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ACADEMY OF ROMANIAN SCIENTISTS<br />

A N N A L S<br />

SERIES ON SCIENCE AND TECHNOLOGY OF INFORMATION<br />

VOLUME 5 2012 NUMBER 1<br />

ONLINE EDITION<br />

ISSN 2066 - 8562<br />

TOPICS:<br />

INFORMATION THEORY AND COMPLEXITY<br />

PHOTONICS AND OPTICAL ENGINEERING<br />

ELECTRONICS AND TELECOMMUNICATIONS<br />

I N F O R M A T I C S A N D C O M P U T E R S<br />

IT SYSTEMS, MECHATRONICS AND ROBOTICS<br />

ADVANCED MATERIALS, NANOSCIENCES AND<br />

NANOTECHNOLOGIES<br />

MICROELECTRONICS AND MICROSYSTEMS<br />

E d i t u r a<br />

ACA DEMIEI OAMENI LO R DE ȘTII NȚĂ DI N ROM ÂNIA<br />

B u c u r e ş t i


A N N A L S O F T H E A C A D E M Y<br />

O F R O M A N I A N S C I E N T I S T S<br />

Series on S C I E N C E A N D T E C H N O L O G Y O F I N F O R M A T I O N<br />

C O N T E N T S<br />

NECULAI ANDREI<br />

THE QUADRUPLED RATIONAL INTERPRETATION OF DIVINITY .................................................. 7<br />

STEFAN IANCU<br />

MAN, MACHINES AND CONSCIENCE? ....................................................................................... 15<br />

I. TUNARU, R. WIDENHORN, E. BODEGOM, D. IORDACHE<br />

COMPUTATIONAL APPROACH TO DARK CURRENT SPECTROSCOPY IN CCD<br />

AS COMPLEX SYSTEMS.PART III. DEFINITION AND USE OF A NEW PARAMETER<br />

CHARACTERIZING THE DEPLETION DARK CURRENT IN SEMICONDUCTORS ............................ 37<br />

ADRIAN SIMION, STEFAN TRAUSAN-MATU<br />

AUTOMATIC COMPUTER MUSIC CLASSIFICATION AND SEGMENTATION................................. 59<br />

CORNEL COBIANU, BOGDAN SERBAN<br />

POLYMERIC PRESSURE SENSORS: A CONCEPTUAL VIEW .......................................................... 75<br />

CATALIN SPULBER, OCTAVIA BORCAN<br />

AN ANALYSIS REGARDING THE DECREASING OF THE IMAGE QUALITY<br />

WITH THE OPTICAL MISALIGNMENT ......................................................................................... 85<br />

BOGDAN-ADRIAN STEFANESCU, DAN ANGHEL, OCTAVIAN DANILA,<br />

PAUL STERIAN, ANDREEA RODICA STERIAN<br />

APPLICATIONS OF QUANTUM CRYPTOLOGY FOR DATA TRANSMISSIONS<br />

IMPLEMENTED IN A STUDENT LABORATORY ............................................................................ 95<br />

DAN ALEXANDRU IORDACHE<br />

THE MATHEMATICAL THEORY OF COMMUNICATIONS VERSUS THE PHYSICAL<br />

THEORY OF INFORMATION. THE UNIVERSE VERSUS THE MULTIVERSE ................................... 109<br />

M.R. JAFARI, M.R. ZARRABI, S. EFFATI<br />

CHAOS AND STABILIZATION OF SELF-REMISSION TUMOR SYSTEM BY SLIDING MODE ........... 125<br />

ONLINE EDITION<br />

Copyright©E d i t u r a A C A D E M I E I O A M E N I L O R D E Ș T I I N Ț Ă D I N R O M Â N I A , 2012


A N N A L S O F T H E A C A D E M Y<br />

O F R O M A N I A N S C I E N T I S TS<br />

Series on S C I E N C E A N D T E C H N O L O GY O F I N F O R M A T I O N<br />

Foun<strong>din</strong>g Editor-in-Chief<br />

Gen. (r) Pr<strong>of</strong>. univ., M.D. Ph.D., Dr. H.C. VASILE CÂNDEA<br />

Foun<strong>din</strong>g, Full Member <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

P r e s i d e n t o f t h e A c a d e m y o f R o m a n i a n S c i e n t i s t s<br />

Co-Editor<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. ADRIAN RUSU<br />

C o r r e s p o n d i n g M e m b e r o f t h e R o m a n i a n A c a d e m y<br />

F u l l M e m b e r o f t h e Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series Editor<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. PAUL STERIAN<br />

F u l l M e m b e r o f t h e Aca<strong>de</strong>my <strong>of</strong> Romanian S c i e n t i s t s<br />

Presi<strong>de</strong>nt <strong>of</strong> the Section Science and Technology <strong>of</strong> Information<br />

Series Editorial Board<br />

Senior Res. Ph.D. Eng. Neculai ANDREI, Research Institute for Informatics, Bucharest<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Mircea BODEA, University “Politehnica” <strong>of</strong> Bucharest<br />

Pr<strong>of</strong>. univ. Ph.D. Erik BODEGOM, Portland State University, Oregon, USA<br />

Pr<strong>of</strong>. univ Ph.D. Eng. Gheorghe BREZEANU, University “Politehnica” <strong>of</strong> Bucharest<br />

Senior Res. Ph.D. Eng. Ştefan CANTARAGIU, UTI Group, Bucharest, Romania<br />

Pr<strong>of</strong>. univ. Ph.D. Carlo CATTANI, University <strong>of</strong> Salerno, Italy<br />

Senior Res. Ph.D. Eng. Cornel COBIANU, Honeywell Romania<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Ştefan IANCU, Romanian Aca<strong>de</strong>my<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Ciprian ILIESCU, Institute <strong>of</strong> Bioengineering<br />

and Nanotechnology, Singapore<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Adrian IONESCU, École Polytechnique Fédérale <strong>de</strong> Lausanne<br />

Pr<strong>of</strong>. univ. Ph.D. Ole KELLER, Department <strong>of</strong> Physics and Nanotechnology,<br />

Aalborg University, Denmark<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Adrian PODOLEANU, Applied Optics Group, University <strong>of</strong> Kent, UK<br />

Senior Res. Ph.D. Eng. Cătălin SPULBER, S.C. Pro Optica S.A., Bucharest<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Ştefan TRĂUŞAN-MATU, University “Politehnica” <strong>of</strong> Bucharest<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Florin UDREA, Engineering Department, University <strong>of</strong> Cambridge, UK<br />

Chief <strong>of</strong> Department: Mihai CĂRUȚAȘU, Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists Publishing House, eng.<br />

Redactor: Andrei D. PETRESCU, Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists Publishing House, pr<strong>of</strong>. National College<br />

“Gheorghe Lazăr”, Ph.D., University „Politehnica” <strong>of</strong> Bucharest, Romania<br />

Documentalist: Ioan BALINT, Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists Publishing House, eng.<br />

The series is published by the section Science and Technology <strong>of</strong> Information <strong>of</strong> the<br />

A c a d e m y o f R o m a n i a n S c i e n t i s t s<br />

Copyright © Editura Aca<strong>de</strong>miei <strong>Oamenilor</strong> <strong>de</strong> Știință <strong>din</strong> România, 2012<br />

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3<br />

FOREWORD<br />

Based on a rich scientific tradition, the Aca<strong>de</strong>my <strong>of</strong><br />

Romanian Scientists, ARS is the continuator and the<br />

unique heir <strong>of</strong> the Romanian Aca<strong>de</strong>my <strong>of</strong> Sciences (1936-<br />

1948). Then, together with the Aca<strong>de</strong>my <strong>of</strong> Medical<br />

Sciences and the Romanian Aca<strong>de</strong>my, it was inclu<strong>de</strong>d (by<br />

Decree <strong>of</strong> the Great National Assembly) into the Aca<strong>de</strong>my<br />

<strong>of</strong> the Romanian Popular Republic, with Aca<strong>de</strong>mician<br />

Traian Savulescu as presi<strong>de</strong>nt.<br />

In 1956, Aca<strong>de</strong>mician Traian Savulescu, together<br />

with other <strong>scientists</strong> and members <strong>of</strong> the Aca<strong>de</strong>my, created<br />

the Association <strong>of</strong> the Romanian Scientists, as a partial<br />

compensation for the disappearance <strong>of</strong> the Romanian<br />

Aca<strong>de</strong>my <strong>of</strong> Sciences. In 1996, at the first National<br />

Congress <strong>of</strong> the Romanian Scientists (with international<br />

participation) the <strong>de</strong>nomination Aca<strong>de</strong>my <strong>of</strong> Romanian<br />

Scientists was adopted, with the same acronym and the<br />

same statute as in 1936.<br />

By the Decree 52, from January 12, 2007, ARS was<br />

recognized as an institution <strong>of</strong> public interest, situated<br />

between the Romanian Aca<strong>de</strong>my and the specialized<br />

Aca<strong>de</strong>mies and enjoying the status <strong>of</strong> chief accountant <strong>of</strong><br />

public funds.<br />

The Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

reappeared and continued, during 2006-2007, the tradition<br />

from 1936, with one volume every year. Starting with<br />

2008, the Annals are published observing the internationally<br />

recognized standards as several in<strong>de</strong>pen<strong>de</strong>nt<br />

series, for each section <strong>of</strong> ARS.<br />

Copyright © Editura Aca<strong>de</strong>miei <strong>Oamenilor</strong> <strong>de</strong> Știință <strong>din</strong> România, 2012<br />

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4<br />

Despite their great diversity, all published papers<br />

must have something in common. They will be assessed by<br />

our referees, trusted researchers in their fields <strong>of</strong> activity<br />

and they must be able to prove be influential in the science<br />

progress.<br />

In essence, we are seeking for papers <strong>of</strong> the highest<br />

quality that present an important advance in conceptual<br />

un<strong>de</strong>rstan<strong>din</strong>g to provi<strong>de</strong> new insights into related<br />

processes or report a new level <strong>of</strong> technological<br />

performance or functionality for the future <strong>de</strong>velopment<br />

in different fields <strong>of</strong> interest.<br />

In the same time, the papers must <strong>of</strong>fer broad appeal<br />

to the scientific community, inclu<strong>din</strong>g the young <strong>scientists</strong><br />

also. I would like, on this occasion to say a big thank-you to<br />

all members <strong>of</strong> the scientific community who either<br />

submitted papers, or acted as referees, or intend to<br />

participate in the future at the success <strong>of</strong> the ARS Annals.<br />

It is my real pleasure to congratulate now the<br />

members <strong>of</strong> the Science and Technology <strong>of</strong> Information<br />

Section <strong>of</strong> ARS and the members <strong>of</strong> the Editorial Board for<br />

continuing the series on Science and Technology <strong>of</strong><br />

Information <strong>of</strong> the Annals. To all <strong>of</strong> them and to the<br />

technical staff involved in the production <strong>of</strong> the journal,<br />

my sincere thanks for their work and my best wishes <strong>of</strong><br />

success in the future activity.<br />

Gen.(r), Pr<strong>of</strong>. univ., M.D., Ph.D., Dr. H.C., Vasile Cân<strong>de</strong>a<br />

Presi<strong>de</strong>nt <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Copyright © Editura Aca<strong>de</strong>miei <strong>Oamenilor</strong> <strong>de</strong> Știință <strong>din</strong> România, 2012<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066 - 8562 Volume 5, Number 1/2012 5<br />

C O N T E N T S<br />

1. Neculai ANDREI<br />

The Quadrupled Rational Interpretation <strong>of</strong> Divinity ........................ 7<br />

2. Stefan IANCU<br />

Man, Machines and Conscience? ............................................................. 15<br />

3. I. TUNARU, R. WIDENHORN, E. BODEGOM, D. IORDACHE<br />

Computational Approach to Dark Current Spectroscopy in CCD as<br />

Complex Systems. Part III. Definition and Use <strong>of</strong> a New Parameter<br />

Characterizing the Depletion Dark Current in Semiconductors ........... 37<br />

4. Adrian SIMION, Stefan TRAUSAN-MATU<br />

Automatic Computer Music Classification and Segmentation ................. 53<br />

5. Cornel COBIANU, Bogdan SERBAN<br />

Polymeric Pressure Sensors: A Conceptual View ................................... 69<br />

6. Catalin SPULBER, Octavia BORCAN<br />

An Analysis Regar<strong>din</strong>g the Decreasing <strong>of</strong> the Image Quality<br />

with the Optical Misalignment ................................................................. 83<br />

7. Bogdan-Adrian STEFANESCU, Dan ANGHEL, Octavian DANILA,<br />

Paul STERIAN, Andreea Rodica STERIAN<br />

Applications <strong>of</strong> Quantum Cryptology for Data Transmissions<br />

Implemented in a Stu<strong>de</strong>nt Laboratory .................................................... 93<br />

Copyright © Editura Aca<strong>de</strong>miei <strong>Oamenilor</strong> <strong>de</strong> Știință <strong>din</strong> România, 2012<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

6 Volume 5, Number 1/2012 ISSN 2066 - 8562<br />

8. Dan Alexandru IORDACHE<br />

The Mathematical Theory <strong>of</strong> Communications versus the Physical<br />

Theory <strong>of</strong> Information. The Universe versus the Multiverse .................... 107<br />

9. M.R. JAFARI, M.R. ZARRABI, S. EFFATI<br />

Chaos and Stabilization <strong>of</strong> Self-Remission Tumor System<br />

by Sli<strong>din</strong>g Mo<strong>de</strong> .......................................................................................... 123<br />

Referents:<br />

Senior Res. Ph.D. Eng. Neculai Andrei<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Mircea Bo<strong>de</strong>a<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Gheorghe Brezeanu<br />

Senior Res. Ph.D. Eng. Ştefan Cantaragiu<br />

Senior Res. Ph.D. Eng. Cornel Cobianu<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Ştefan Iancu<br />

Senior Res. Ph.D. Eng. Mircea Valer Puşcă<br />

Senior Res. Ph.D. Eng. Cătălin Spulber<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Paul Sterian<br />

Pr<strong>of</strong>. univ. Ph.D. Eng. Ştefan Trăuşan-Matu<br />

Copyright © Editura Aca<strong>de</strong>miei <strong>Oamenilor</strong> <strong>de</strong> Știință <strong>din</strong> România, 2012<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066 - 8562 Volume 4, Number 2/2011 7<br />

THE QUADRUPLED RATIONAL INTERPRETATION<br />

OF DIVINITY<br />

Neculai ANDREI 1<br />

Abstract. When speaking about the rational interpretation <strong>of</strong> Divinity, there are three<br />

main concepts that we will briefly summarize in this paper. At the end <strong>of</strong> it we will present<br />

a fourth one, namely the symmetric rational interpretation <strong>of</strong> Divinity, as well as the<br />

connections between it and the other three ones.<br />

Keywords: Tzimtzum concept, Coinci<strong>de</strong>ntia Oppositorum concept, Continuous Creation concept,<br />

Symmetry Concept, Mathematical mo<strong>de</strong>ling, Occam's razor<br />

1. Introduction<br />

We should mention that the first three concepts belong to the Western World, to<br />

the Catholic Church, which for more than 1000 years has ma<strong>de</strong> a constant effort<br />

for reconciliation between Aristotle (384-322 B.C.) and the Christian Dogma.<br />

We, the Romanians, and actually the entire Eastern world, did not have a<br />

Renaissance age, in the general meaning <strong>of</strong> the concept.<br />

We did not need Renaissance. We had the Holly Eastern Fathers, whose effort<br />

surpassed ancient art and philosophy and gave answers to the fundamental<br />

problems <strong>of</strong> the human condition, answers that did not involve their issuing <strong>of</strong><br />

philosophical systems.<br />

2. The Tzimtzum Concept<br />

The most serious attempt to explain the i<strong>de</strong>a <strong>of</strong> Creation ex nihilo is expressed in<br />

the theology <strong>of</strong> Isaac Luria (Arizaal) (1534-1572). Consi<strong>de</strong>red as being the<br />

foun<strong>de</strong>r <strong>of</strong> New Kabbalah, in fact the greatest Kabbalist <strong>of</strong> all times, he uses the<br />

Tzimtzum doctrine - concentration, contraction or withdrawal. Being an<br />

intellectual concept <strong>of</strong> Jewish mysticism, Kabbalah is an area <strong>de</strong>alt with not only<br />

by Hebrew scholars. Kabbalah does not give much importance to the primordial<br />

chaos. It conceives the world as an organized system, something that, in the<br />

current language, would be consi<strong>de</strong>red a system governed by laws (conservation<br />

laws) and not by hazard. Kabbalah is essentially a system representing the world<br />

through areas <strong>of</strong> perception and representation, <strong>of</strong> interpretation <strong>of</strong> Divinity.<br />

Accor<strong>din</strong>g to Luria, the existence <strong>of</strong> the Universe was possible only through a<br />

process <strong>of</strong> "contraction" <strong>of</strong> God, i.e.<br />

1 Research Institute for Informatics, Centre for Advanced Mo<strong>de</strong>lling and Optimization, 8-10,<br />

Averescu Avenue, Bucharest 1,. Full member <strong>of</strong> the Romanian Aca<strong>de</strong>my. (e-mail: nandrei@ici.ro).<br />

Copyright © Editura Aca<strong>de</strong>miei <strong>Oamenilor</strong> <strong>de</strong> Știință <strong>din</strong> România, 2012<br />

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8 Neculai Andrei<br />

”After Genesis, God, keeping intact His essence, has retired within Himself to<br />

make way for the world itself, leaving, so to speak, an area insi<strong>de</strong> Him, some<br />

sort <strong>of</strong> mystical space from which He withdrew in or<strong>de</strong>r to return to the acts <strong>of</strong><br />

creation and <strong>of</strong> revelation” [Scholem, 1960], [Elia<strong>de</strong>, 2000, p. 577].<br />

In this view, God's withdrawal is more than a metaphor. It is rather a change in<br />

His intensity over the world.<br />

Notice that there are two forms <strong>of</strong> Tzimtzum, two forms <strong>of</strong> withdrawal. The first<br />

one relates to the withdrawal <strong>of</strong> the divine being in itself in or<strong>de</strong>r to allow the<br />

existence <strong>of</strong> the physical world. The second one is the withdrawal <strong>of</strong> the "divine<br />

will" in or<strong>de</strong>r to confer freedom <strong>of</strong> choice to the human being. However, this<br />

meant sacrifying the unity and exclusivity <strong>of</strong> Divinity. Therefore, the Tzimtzum<br />

concept within Kabbalah states that the existence <strong>of</strong> free-will was conditioned by<br />

the <strong>de</strong>struction <strong>of</strong> the original or<strong>de</strong>r, <strong>of</strong> the unity and symmetry, which are<br />

fundamental attributes <strong>of</strong> Divinity.<br />

Creating the Universe and making the free-will efficient implied giving up the<br />

fundamental principle <strong>of</strong> science, that <strong>of</strong> causality. At this moment, Tzimtzum is<br />

the only place where the principle <strong>of</strong> causality is not satisfied. This <strong>de</strong>fines and<br />

explains the "singularity" mentioned in the Big Bang theory (please see paragraph<br />

4 below), an exception that does not need the principle <strong>of</strong> causality. The unity <strong>of</strong><br />

natural laws, their ubiquity in the sense that "The universe is full <strong>of</strong> laws" arises<br />

from the unity <strong>of</strong> the Divine being, <strong>of</strong> Almighty, and from the Divine will. Giving<br />

up the principle <strong>of</strong> causality in the act <strong>of</strong> creating the physical Universe and the<br />

free will becomes therefore similar to the "withdrawal <strong>of</strong> God", to Tzimtzum.<br />

Luria's Kabbalah is the greatest victory achieved by the anthropomorphic<br />

philosophical trend in the history <strong>of</strong> Rabbinic Judaism and Hebrew mysticism, the<br />

last religious movement with influence in all Hebrew environments and in all<br />

countries without exception [Scholem, 1960]. Its significance, as manifestation <strong>of</strong><br />

rationality aiming at clarifying the act <strong>of</strong> the creation <strong>of</strong> the Universe and <strong>of</strong> the<br />

free will, emerges as well from the fact that Tzimtzum, as the essence <strong>of</strong><br />

Kabbalah, is entirely present in the mo<strong>de</strong>rn cosmological theory <strong>of</strong> the Big Bang.<br />

3. The Coinci<strong>de</strong>ntia Oppositorum Concept<br />

A second concept in the rational interpretation <strong>of</strong> Divinity is closely related to the<br />

problem <strong>of</strong> conjecture and was <strong>de</strong>alt with by the German Bishop Nicholas <strong>of</strong> Cusa<br />

(1401-1464) in his remarkable work De Docta Ignorantia (Of Learned Ignorance),<br />

written in 1440. The theme <strong>of</strong> this original but difficult work is that most <strong>of</strong> our<br />

knowledge is a conjecture, and admitting this is a matter <strong>of</strong> wisdom.<br />

Accor<strong>din</strong>g to this concept, Cusa's universe is an expression that is an imperfect and<br />

ina<strong>de</strong>quate explanation (explicatio) <strong>of</strong> God, because this explanation occurs within<br />

Copyright © Editura Aca<strong>de</strong>miei <strong>Oamenilor</strong> <strong>de</strong> Știință <strong>din</strong> România, 2012<br />

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The Quadrupled Rational Interpretation <strong>of</strong> Divinity 9<br />

the sphere field <strong>of</strong> multiplicity and separation. On the other hand, within God, the<br />

universe is present in a strict and indissoluble unity (complicatio), a unity that<br />

inclu<strong>de</strong>s all qualities and <strong>de</strong>terminations, which are not only different, but even<br />

opposite to one being. In Cusa's interpretation, any single being in the universe<br />

represents the universe itself and therefore God himself, in a proprietary manner,<br />

characteristic to that very being, contracting (contractio) the infinite richness <strong>of</strong> the<br />

universe based on the own individuality <strong>of</strong> the being itself.<br />

Cusa, who was the last major philosopher-theologian <strong>of</strong> the Roman Church, one<br />

and inseparable, a "Ianus <strong>of</strong> philosophy" in the interpretation <strong>of</strong> P. P. Negulescu<br />

(1872-1951) because he was pointing on one hand towards the Middle Ages and on<br />

the other hand towards the Renaissance, argues that knowledge, which is relative<br />

and finite, is unable to grasp the truth, which is simple and infinite. A great<br />

personality <strong>of</strong> his time, Nicholas <strong>of</strong> Cusa, until he met Plethon Gemistos Georgios<br />

(1355-1452) during a trip to Byzantium (1437) to attend a church council, was<br />

oriented towards the Renaissance, a new world which was just being born. The<br />

meeting with Plethon, a Greek Neo-Platonist philosopher who had come to Italy<br />

and stirred in Florence a great movement <strong>of</strong> i<strong>de</strong>as that would later lead to the<br />

foun<strong>din</strong>g <strong>of</strong> "Acca<strong>de</strong>mia Platonica" <strong>of</strong> Florence by Marsiglio Ficino (1433-1499),<br />

also <strong>de</strong>termined Cusa's return toward the prevailing mentality <strong>of</strong> the Middle Ages.<br />

The outstan<strong>din</strong>g all-reaching perspective <strong>of</strong> his metaphysics can be noticed in his<br />

exceptional works De Concordantia Catholica (1434) and De Pace Fi<strong>de</strong>i (On the<br />

Peace <strong>of</strong> Faith - 1453) in response to the fall <strong>of</strong> Constantinople un<strong>de</strong>r the Turks. In<br />

these works, Cusa <strong>de</strong>fines concordantia as a universal theme. The bold conclusion<br />

he reaches, concordantia, is drawn with aid from negative theology. Using the<br />

same approach he comes to his masterpiece, De Docta Ignorantia.<br />

Any science being conjectural, man himself cannot<br />

know God. The truth - the absolute maximum - is<br />

beyond reason because reason is unable to solve<br />

contradictions. One must, therefore, transcend beyond<br />

discursive reason and imagination and get maximum<br />

<strong>of</strong> wisdom through intuition. But since the intellect<br />

cannot express itself using a rational language, Cusa<br />

resorts to symbols and, before anything else, to<br />

geometric figures.<br />

Within God, that which is infinitely large (maximum)<br />

coinci<strong>de</strong>s with that which is infinitely small<br />

(minimum) and virtuality coinci<strong>de</strong>s with action. In Nicolas <strong>of</strong> Cusa (1401-1464).<br />

His infinite simplicity, God hi<strong>de</strong>s (complicato) all<br />

things, but at the same time He is in all things (explicato); i.e., complicato<br />

coinci<strong>de</strong>s with explicato, which is the coinci<strong>de</strong>ntia oppositorum principle. By<br />

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10 Neculai Andrei<br />

un<strong>de</strong>rstan<strong>din</strong>g this principle, our ”ignorance” becomes ”erudite”. Still,<br />

coinci<strong>de</strong>ntia oppositorum must not be interpreted as a synthesis gained through<br />

reasoning, because it cannot be achieved in terms <strong>of</strong> finitu<strong>de</strong>, but in a manner <strong>of</strong><br />

conjecture, in the infinite plane [Elia<strong>de</strong>, 2000, p. 599-600].<br />

This is an exceptional interpretation <strong>of</strong> Divinity, comparable to that given by Isaac<br />

Luria in his New Kabbala.<br />

”By knowing in part” as Apostle Paul taught us in his First Epistle to the<br />

Corinthians (Chapter 13, verse 9) and without access to ultimate truths we can<br />

only make conjectures. As long as they withstand the tests, they are accepted.<br />

Otherwise, they are rejected, leaving room for other theories to replace them and<br />

summarize their experience.<br />

4. The Continuous Creation Concept<br />

Still, the most elaborate concept in the rational interpretation <strong>of</strong> Divinity belongs<br />

to Descartes. Descartes' philosophy starts <strong>of</strong>f with cogito, and it starts from the<br />

fact that ”I think” is an indisputable fin<strong>din</strong>g observed directly, not through<br />

<strong>de</strong>ductions. The next step in Descartes’ philosophy indicates that ”I”, as a<br />

thinking being, am capable <strong>of</strong> certainties and those certainties are obtained by<br />

direct intuition, through direct knowledge. In this respect Descartes, by intuition<br />

and certainty, gives a very solid foundation <strong>of</strong> human subjectivity. Then<br />

Descartes raises the question <strong>of</strong> how to exit from man's inner world outsi<strong>de</strong> into<br />

the objective world in or<strong>de</strong>r to gain knowledge <strong>of</strong> the world around us. His<br />

solution is as follows. By thinking, more specifically, through the lucidity <strong>of</strong><br />

thinking, he reaches another obvious fact, namely the existence itself - cogito,<br />

ergo sum. Thus, the act <strong>of</strong> thinking contains within itself the very existence <strong>of</strong> the<br />

thoughtful subject. In this way, through the existence <strong>of</strong> the thinking subject, the<br />

transition to the outsi<strong>de</strong> world, to the universal world <strong>of</strong> ”to exist” becomes<br />

possible. For Descartes, thinking is primordial to the extent that ”the mind is<br />

better known than the body”.<br />

When Descartes says ”cogito, ergo sum” he does not refer to his existence, but to<br />

his existence as ”thinking matter”, as mind itself, leaving the body as an annex to<br />

be handled some other time. In total agreement with St. Francis <strong>of</strong> Assisi (1181-<br />

1226) who refers to ”his brother, the body”, Descartes realized that in or<strong>de</strong>r to be<br />

strengthened, the formula "cogito, ergo sum" needs to be continued with<br />

something further on. In<strong>de</strong>ed, it is very possible for an evil spirit (malin génie) to<br />

<strong>de</strong>lu<strong>de</strong> and mislead him, so that everything he thinks would become an illusion.<br />

To avoid that, Descartes needs the i<strong>de</strong>a <strong>of</strong> God, whose existence he supports through<br />

the ontological argument, as Anselm <strong>of</strong> Canterbury (1033-1109) did for the first time<br />

500 years before. Thus, Good God is the guarantor <strong>of</strong> all truths, for He is never wrong<br />

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The Quadrupled Rational Interpretation <strong>of</strong> Divinity 11<br />

and, given His nature, He cannot <strong>de</strong>lu<strong>de</strong> us. However, even if we ignore the logical<br />

error contained in the ontological argument, there is another problem that appears<br />

instantly: God guarantees the truths <strong>of</strong> the world, but there are eternal truths - the<br />

truths <strong>of</strong> mathematics. What is then God's relationship with these truths like? Eternal<br />

truths cannot be changed. Therefore is God subject to them?<br />

Descartes gives a masterly solution to this problem<br />

introducing the concept <strong>of</strong> continuous creation: the<br />

free relationship between God and His creation is<br />

the same from the very beginning to the end and it is<br />

a creative connection at every moment. This implies<br />

that, along with the continuous creation which<br />

Descartes attributes to God and parallel with it, the<br />

implicit emergence <strong>of</strong> a continuous doubt keeps<br />

human certainties awake. And so, in its essence,<br />

Descartes's conception contains the universal doubt.<br />

All mo<strong>de</strong>rn culture, all our achievements are based on<br />

doubts and certainties, or as Anton Dumitriu (1905- René Descartes (1596-1650).<br />

1992) [1986] says so beautifully in The Book <strong>of</strong><br />

Admirable Encounters (Cartea întâlnirilor admirabile), in the essay Descartes or<br />

the Endless Doubt: ”on doubts about the doubts and certainties, on doubts about<br />

the doubts and the certainty <strong>of</strong> certainties in a regresus in infinitum, that is to say,<br />

a continuous re-examination <strong>of</strong> all values and certainties”.<br />

5. The concept <strong>of</strong> symmetry<br />

We saw that the rational interpretation <strong>of</strong> Divinity's continuous creation places<br />

God in free relationship with His creation, in a creative relationship that is present<br />

every moment and at every point <strong>of</strong> the Universe.<br />

In the current outlook regar<strong>din</strong>g the formation <strong>of</strong> the Universe known as the Big<br />

Bang theory, proposed by Georges Lemaître (1894-1966), our Universe began its<br />

existence 13.7 billion years ago as a very small singularity, extremely hot and <strong>of</strong><br />

very high <strong>de</strong>nsity. During this period <strong>of</strong> billions and billions <strong>of</strong> years it expan<strong>de</strong>d<br />

and cooled, so as to reach the current size and temperature. The Big Bang theory<br />

is supported by the so-called "Hubble's Law", named after Edwin Hubble (1889-<br />

1953), who, in 1929 discovered that galaxies move further and further from us at a<br />

speed that is proportional with distance. The further a galaxy is from us, the faster<br />

its distancing speed. Objects that are the farthest seem to be moving away from us<br />

with the speed <strong>of</strong> light. Therefore, one may as well assume that at some moment<br />

back in time, the Universe was concentrated in a single spot, with very high<br />

<strong>de</strong>nsity and temperature. We then see that the Universe, being in the beginning<br />

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12 Neculai Andrei<br />

only a spot with the above mentioned properties, was symmetrical, perfectly<br />

symmetrical.<br />

The Big Bang did not happen in space and time. Accor<strong>din</strong>g to the current<br />

acceptance, space and time felt as such were created during the Big Bang. So, to<br />

ask what had been before the Big Bang makes no sense. Meanwhile, it must be<br />

noted that the concepts <strong>of</strong> space and time are characteristics <strong>of</strong> human<br />

consciousness. The human being lives in the past, present and future. Only the<br />

Divine is in a perpetual present.<br />

One remarkable aspect <strong>of</strong> this cosmogonist theory is the following: as we go back<br />

in time the Universe gets hotter, <strong>de</strong>nser and the symmetries, now <strong>de</strong>stroyed, are<br />

restored. In other words, while going back in time towards the Big Bang moment,<br />

the Universe and the interactions between particles become increasingly<br />

symmetrical. This shows that the Universe becomes more simple and symmetrical.<br />

In a somehow more simple way, without making much <strong>of</strong> a mistake, we can say<br />

that life is organised matter or energy, based on differentiation. If the Universe is<br />

perfectly symmetrical and uniform and totally or<strong>de</strong>red, then within this Universe<br />

there is no complexity, no structure can be i<strong>de</strong>ntified, no form <strong>of</strong> life, no<br />

consciousness. In other words, in a perfectly symmetrical and uniform Universe,<br />

as it was at the moment <strong>of</strong> the Big Bang, life and consciousness were not possible.<br />

In the general acceptance <strong>of</strong> the Big Bang we see that the Universe was originally<br />

a point containing an amorphous, relatively uniform energy mixture. This<br />

uniformity was <strong>de</strong>stroyed with the start <strong>of</strong> expansion and the energy transformed<br />

itself into a mixture <strong>of</strong> elementary particles. As the Universe expan<strong>de</strong>d, these<br />

particles packed, forming galaxies with stars and planets and other celestial<br />

bodies. As the differentiation grew steep and the initial or<strong>de</strong>r was <strong>de</strong>stroyed, the<br />

structure and complexity <strong>of</strong> the Universe increased. In the end, the differentiation<br />

was broad enough to inbreed living things, brain and consciousness. In other<br />

words, life can appear only in a Universe in which symmetry is not total, and this<br />

can continue only by transforming the pre-existing or<strong>de</strong>r into chaos.<br />

Given the balance that exists in the Universe as well as the uniformity <strong>of</strong> the<br />

cosmic background radiation and the luminescence that fills the Universe, its<br />

expansion evolves in a homogeneous and isotropic way. That is to say, the<br />

expansion <strong>of</strong> the Universe has no privileged directions. Therefore, at the moment<br />

<strong>of</strong> the Big Bang, the Universe, which was only one point, a singularity, was<br />

<strong>de</strong>stroyed in an infinite number <strong>of</strong> symmetries, but at the same time, given the<br />

homogeneity and isotropy <strong>of</strong> the Universe, on another level, the original<br />

symmetry has been preserved. So the essential and remarkable aspect <strong>of</strong> our<br />

Universe is that <strong>of</strong> preserving the symmetry at a global level (the macroscopicscale,<br />

the entire Universe), as well as locally, in the sense that at any time and at<br />

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The Quadrupled Rational Interpretation <strong>of</strong> Divinity 13<br />

any place we are surroun<strong>de</strong>d by concepts that arise in dual-symmetric pairs, i.e.<br />

we are immersed in an ocean <strong>of</strong> symmetries. And so, the concept <strong>of</strong> continuous<br />

creation completes and reinforces itself as the following rational interpretation <strong>of</strong><br />

Divinity: God's free relationship with His creation is the same from the very<br />

beginning to the end, that is, a continuous creative relationship in dualsymmetric<br />

concepts at any moment.<br />

6. Fundamentals <strong>of</strong> mathematical mo<strong>de</strong>ling<br />

Mathematical mo<strong>de</strong>ling is an activity <strong>of</strong> high intellectualism through which a<br />

certain part <strong>of</strong> the Universe is represented in mathematical symbols. The goal <strong>of</strong><br />

mathematical mo<strong>de</strong>ling is to build a mathematical tool that would provi<strong>de</strong> the<br />

un<strong>de</strong>rstan<strong>din</strong>g <strong>of</strong> the movement which takes place in the part <strong>of</strong> the Universe we are<br />

interested in and to make accurate predictions <strong>of</strong> its evolution. Mathematical mo<strong>de</strong>ls<br />

are presented in a variety <strong>of</strong> forms. The most important seem to be: linear or nonlinear,<br />

<strong>de</strong>terministic or stochastic, static or dynamic, discrete or continuous, etc.<br />

They come in any shape, all <strong>of</strong> them satisfying the principle <strong>of</strong> causality.<br />

Mathematical mo<strong>de</strong>ls are written based on<br />

conservation laws that represent the essence <strong>of</strong> the<br />

Universe. These, in turn, as <strong>de</strong>monstrated by Emmy<br />

Noether (1882-1935), arise from symmetries, which<br />

form the basis <strong>of</strong> our knowable Universe. Being<br />

surroun<strong>de</strong>d by an ocean <strong>of</strong> dual-symmetrical paired<br />

concepts, the result is that the conservation laws<br />

have a very serious base that ensures the a<strong>de</strong>quacy<br />

<strong>of</strong> mathematical mo<strong>de</strong>ls. In this respect Descartes’<br />

view <strong>of</strong> continuous creation is completed in the<br />

sense that, the free relationship <strong>of</strong> God with His<br />

creation continuously creates symmetrical concepts.<br />

The complexity <strong>of</strong> a given mo<strong>de</strong>l always involves<br />

equilibrium, a balance between its simplicity and its<br />

Emmy Noether (1882-1935)<br />

accuracy in representation. What is important here is Occam's razor: out <strong>of</strong> the<br />

mo<strong>de</strong>ls that have the same power <strong>of</strong> representation and prediction, it is<br />

recommen<strong>de</strong>d that the simplest should be chosen.<br />

The i<strong>de</strong>a is that the mo<strong>de</strong>l should be as simple as possible, but not simplistic.<br />

Increasing the complexity <strong>of</strong> a mo<strong>de</strong>l improves its realism, therefore its power <strong>of</strong><br />

representation, but it creates difficulties in un<strong>de</strong>rstan<strong>din</strong>g and analyzing the mo<strong>de</strong>l<br />

and raises computational questions about the size <strong>of</strong> the mo<strong>de</strong>l and about the<br />

numerical instabilities in the solving process. Therefore, a mathematical mo<strong>de</strong>l, in<br />

the perspective <strong>of</strong> infinite similarities with reality, is characterized by simplicity<br />

imposed by conservation laws.<br />

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14 Neculai Andrei<br />

R E F E R E N C E S<br />

[1] Andrei, N., (2006) Eseu asupra fundamentelor informaticii. Editura Yes, Bucureşti, 2006.<br />

[2] Andrei, N., (2009) The Pre-eminence <strong>of</strong> Existence versus the Pre-eminence <strong>of</strong> Mathematics,<br />

November 2, 2009. [http://camo.ici.ro/neculai/n47a09. pdf].<br />

[3] Andrei, N., (2009) Aspecte ale evoluției filos<strong>of</strong>iei și a științei. Mai 4, 2009.<br />

[http://camo.ici.ro/neculai/n31a09.pdf]<br />

[4] Andrei, N., (2011) Împătrita interpretare raţională a Divinităţii, Manuscript, June 8, 2011.<br />

[http://camo.ici.ro/neculai/r10a11.pdf]<br />

[5] Curley, E.M., (1984) Descartes on the creation <strong>of</strong> the eternal truths. The Philosophical<br />

Review, vol.93, No.4, (Oct. 1984), pp. 569-597.<br />

[6] Dumitriu, A., (1986) Eseuri. Ştiinţă şi Cunoaştere. Alétheia. Cartea Întâlnirilor Admirabile.<br />

Editura Eminescu, Bucureşti, 1986.<br />

[7] Elia<strong>de</strong>, M., (2000) Istoria Cre<strong>din</strong>ţelor şi I<strong>de</strong>ilor Religioase, Editura Univers Enciclopedic,<br />

Bucureşti, 2000. (Traducere şi postfaţă <strong>de</strong> Cezar Baltag.)<br />

[8] Matthew McMahon, C., The Doctrine <strong>of</strong> Continuous Creation.<br />

[http://www.apuritansmind.com/ChristianWalk/McMahonDoctrineContinuousCreation.htm]<br />

[9] Scholem, G., (1960) Major Trends in Jewish Mysticism, New York, 1946, (ediţia 4,<br />

revizuită şi adăugită, cu bibliografie suplimentară), 1960.<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066 - 8562 Volume 5, Number 1/2012 15<br />

MAN, MACHINES AND CONSCIENCE?<br />

Stefan IANCU 1<br />

Abstract. This paper presents a summary <strong>of</strong> the impact that the impetuous <strong>de</strong>velopment <strong>of</strong><br />

information science and technology may have, emphasizing the trends and the role <strong>of</strong> artificial<br />

intelligence. It sets out what conscience is, the way in which the information is processed in<br />

the system <strong>of</strong> human thought, which is the relationship between this system and the study <strong>of</strong><br />

human conscience and the way in which man-to-man, man-to-machine and machine-tomachine<br />

intercommunication is ma<strong>de</strong>. Then some controversial views on the possibility <strong>of</strong> the<br />

existence <strong>of</strong> some machines with conscience are presented and it is <strong>de</strong>monstrated why it is not<br />

possible to build such machines in the near future. The conclusion is that, in the near future,<br />

machines with a conscience are not consistent with reality and that the best thing would be to<br />

state that it will be possible in the future to build machines not with human intelligence, but<br />

only machines with algorithmic, binary intelligence.<br />

Keywords: artificial intelligence, conscience, intercommunication<br />

1. Introduction<br />

“Man, know thyself and thou wilt know<br />

the Universe and the Gods”<br />

Inscription from the frontispiece <strong>of</strong> the Temple <strong>of</strong> Delphi.<br />

Information science and technology 2 is one <strong>of</strong> the rapidly evolving areas with the<br />

most spectacular implications on the economic and social life. However, there are<br />

some serious reasons to believe that what we have seen so far only its beginning.<br />

Artificial intelligence is an important factor in the evolution <strong>of</strong> information science<br />

and technology. This intelligence makes each element, <strong>de</strong>vice, component or<br />

1 Pr<strong>of</strong>. PhD. Eng., Scientific Secretary <strong>of</strong> the Information Science and Technology Department <strong>of</strong> the<br />

Romanian Aca<strong>de</strong>my, Scientific Secretary <strong>of</strong> the Romanian Committee for the History and Philosophy<br />

<strong>of</strong> Science and Technique from the Romanian Aca<strong>de</strong>my, Full, foun<strong>din</strong>g member <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong><br />

Romanian Scientists.<br />

2 For the enunciation <strong>of</strong> the new scientific achievements in the field <strong>of</strong> automated information<br />

processing the Europeans have promoted the term computer science (<strong>de</strong>signed by the French in<br />

1964) and the Americans have oscillated between “Computer Science” for the theoretical aspects<br />

and ,,Electronic Data Processing” for the applicative, practical aspects. The term information<br />

technology, which has become wi<strong>de</strong>ly accepted today, is relatively new and marks a maturation <strong>of</strong><br />

the field which has excee<strong>de</strong>d the stage <strong>of</strong> science and craft, entering the industrial phase. As the<br />

technology <strong>of</strong> automated information processing generalized beyond the scope <strong>of</strong> numerical<br />

calculation, the data and the computer are no longer perceived as essential (nowadays, the<br />

potential visit to a virtual museum seems to have no connection with the earlier introduction <strong>of</strong><br />

data with punched tape to calculate wages or prices). In addition, the term information technology<br />

shows symmetry with communication technology, <strong>of</strong>fering the possibility <strong>of</strong> a linguistic<br />

integration in the term information and communication technology with the acronym ICT.<br />

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16 Stefan Iancu<br />

system perform these three steps for any given task: to assess its internal conditions<br />

and performance; to <strong>de</strong>termine the requirements <strong>of</strong> any given task and if there is a<br />

correlation between the conclusions <strong>of</strong> the first two stages, to <strong>de</strong>termine what to do:<br />

if there is a correspon<strong>de</strong>nce it executes it, if not it seeks help.<br />

The interaction between microelectronics and the new “photonic” 1 science and<br />

Nanochemistry 2 and biotechnology shows the importance <strong>of</strong> ISoC (Intelligent<br />

Systems on a Chip) technology to human evolution. This technology will create<br />

conditions for obtaining intelligent systems built on a single chip (ISoC).<br />

ISoC technology is consi<strong>de</strong>red the top innovative process that will allow the<br />

integration <strong>of</strong> the latest technological knowledge, selected from the intelligent<br />

computer networks. It will make possible the <strong>de</strong>velopment <strong>of</strong> some new circuits<br />

and new intelligent systems with extraor<strong>din</strong>ary features relevant to all the<br />

economic sectors. Intelligent systems built on a single chip can be applied in areas<br />

such as: health monitoring, medical diagnosis, microsurgery, Nano chemistry,<br />

environmental monitoring, etc. (Iancu St., 2007).<br />

Recently, the similarity between man and machine has been increasingly <strong>de</strong>bated<br />

in the literature, the man being consi<strong>de</strong>red a sophisticated machine ma<strong>de</strong> <strong>of</strong><br />

billions <strong>of</strong> biomoleculars that interact in accordance with the rules <strong>de</strong>rived from<br />

science, presumed to be well <strong>de</strong>fined, but which are still incompletely known<br />

(Brooks Rodney, 2008). These biomoleculars interactions in our head generate<br />

our mind and our intelligence, our feelings and emotions, the consciousness <strong>of</strong> our<br />

existence. Accepting these assumptions would lead to remarkable possibilities. If<br />

we work like machines and if we manage to un<strong>de</strong>rstand and assimilate all these<br />

rules that govern our mind, then, in principle, there should be no reason why we<br />

should not reproduce, in silicon and steel, machinery to operate un<strong>de</strong>r the same<br />

rules by which the man himself operates. Supposedly, these machines should be<br />

able to <strong>de</strong>monstrate that they have human intelligence, human emotions and even<br />

human consciousness. The problem to be clarified is if we work like machines or<br />

not-if it were so-if we can ever i<strong>de</strong>ntify all the rules by which we operate.<br />

Information and communication technology has begun to be incorporated into the<br />

environment and the objects <strong>of</strong> current use; its use is so man "friendly" that it is no<br />

longer seen as an annex, but as a current integral part. In the report "2006 State <strong>of</strong> the<br />

Future" (http://www.acunu.org/millenium/s<strong>of</strong>2006.html), conducted by over 2000<br />

<strong>scientists</strong> and futurists, the increasing interest in the man-machine collective<br />

intelligence, which is expected to grow significantly in the next 25 years, is signaled.<br />

1 Photonic science- the science <strong>of</strong> electronic phenomena based on the propagation <strong>of</strong> light.<br />

2 Nanochemistry - discipline that <strong>de</strong>als with the formation <strong>of</strong> future materials through a better<br />

un<strong>de</strong>rstan<strong>din</strong>g <strong>of</strong> the unique properties <strong>of</strong> atom and molecule sets, ranging in size from that <strong>of</strong> an<br />

individual atom to those <strong>of</strong> some pieces <strong>of</strong> material.<br />

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Man, Machines and Conscience? 17<br />

Un<strong>de</strong>rstan<strong>din</strong>g the brain, the mind and the human consciousness is consi<strong>de</strong>red<br />

today the last frontier <strong>of</strong> science by many <strong>scientists</strong>. In fact, the sciences <strong>of</strong> mind<br />

and consciousness, besi<strong>de</strong>s quantum physics, have reached a common, unique<br />

frontier <strong>of</strong> science (Mihai Draganescu, 2000).<br />

Mind and consciousness cannot be fully explained without quantum physics and<br />

the study <strong>of</strong> the latter will no longer evolve without taking into account the<br />

consciousness. What connects the frontiers <strong>of</strong> quantum physics and consciousness<br />

is the phenomenological information 1 , the “experience”, qualia 2 , the active<br />

information that generates the quantum world accor<strong>din</strong>g to David Bohm 3 , and<br />

generally the phenomenological meanings (Mihai Draganescu, 1999).<br />

2. What is conscience?<br />

The nature <strong>of</strong> consciousness is not yet un<strong>de</strong>rstood and therefore, scientifically,<br />

there is no conclusive answer to the question what is conscience. There is only a<br />

concept that makes connections between individuals and their knowledge on their<br />

own existence.<br />

Conscience is extremely difficult to <strong>de</strong>fine scientifically because it is entirely<br />

subjective. For this reason, its study has long belonged to philosophy and religion.<br />

Recently, the biologists, especially the neurobiologists, have entered the <strong>de</strong>bate.<br />

Some <strong>of</strong> them hoped that the image <strong>of</strong> the brain and the electrical rea<strong>din</strong>g <strong>of</strong> brain<br />

signals will reveal “the neural correlation <strong>of</strong> consciousness” and actually there has<br />

been ma<strong>de</strong> significant progress in this field. But what exactly in our brain activity<br />

1 Phenomenologically - on phenomenology (1.-<strong>de</strong>scriptive study <strong>of</strong> a set <strong>of</strong> phenomena as they<br />

manifest in time and space; 2. - <strong>de</strong>scription / in Fichte and Hegel /<strong>of</strong> the spiritual history <strong>of</strong><br />

conscience that grows from sensorial certainty to "absolute science”; 3.-i<strong>de</strong>alist philosophical<br />

current-established by E. Husserl, which reduces the “object” to “phenomenon”, seen as spiritual<br />

essence and as a final and direct result <strong>of</strong> consciousness, regardless <strong>of</strong> the objective existence and<br />

the sensorial experience.)<br />

2 Qualia come from Latin and it is the plural form, meaning qualities. The singular form quale<br />

means “a certain type” or “a certain way”. In the philosophy <strong>of</strong> mind, the term qualia was used for<br />

the first time in 1929 by Clarence I. Lewis (philosopher, 1883 - 1964) in the paper "Mind and the<br />

World Or<strong>de</strong>r" to <strong>de</strong>scribe the recognizable qualitative characteristics <strong>of</strong> a given fact that should not<br />

be confused with the objective properties <strong>of</strong> the objects in the external world. The term qualia has<br />

been established after 1982 with the publication <strong>of</strong> Frank Jackson’s article (Australian philosopher<br />

b.1943) “Epiphenomenal Qualia”, where it receives the meaning <strong>of</strong> certain features <strong>of</strong> the bodily<br />

sensations and <strong>of</strong> certain perceptual experiences which cannot be reduced to what is inclu<strong>de</strong>d in<br />

the pure physical information. Qualia can also be <strong>de</strong>fined as introspective phenomenal aspect <strong>of</strong><br />

mental states that arise as a result <strong>of</strong> perception, in a certain appropriate manner, <strong>of</strong> the sensations<br />

in an environment. Qualia refer, therefore, to the way in which things appear to us, the way in<br />

which they reach the consciousness through the reception <strong>of</strong> the senses.<br />

3 David Joseph Bohm (20 December 1917-27 October 1992) was a scientist with real<br />

contributions in theoretical physics, philosophy and neuropsychology, as well as in the Manhattan<br />

Project;<br />

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18 Stefan Iancu<br />

makes us be conscious is still unknown. Certainly, there is no area in the brain<br />

that is active only when we are conscious and that is passive when we no longer<br />

realize that we are conscious. Even if we accept (and not everyone does) that it<br />

comes from the brain, there are still some problems. The situation was called “the<br />

hard problem” <strong>of</strong> consciousness, some people trying to explain it by calling it “the<br />

emergent property <strong>of</strong> the active neuronal networks” - something that is born <strong>of</strong> the<br />

interaction between neurons, but not found in them.<br />

Conscience is the most advanced man specific form <strong>of</strong> objective psychological<br />

reflection <strong>of</strong> reality by means <strong>of</strong> sensations, perceptions and thoughts in the form<br />

<strong>of</strong> representations, concepts, judgments, and reasoning, inclu<strong>din</strong>g emotional and<br />

volitional processes. Consciousness is a superior process <strong>of</strong> the human mind,<br />

<strong>de</strong>veloped through social activity and enculturation 1 , by means <strong>of</strong> communication,<br />

based on an internal and internal-external (verbal and written) communication<br />

mo<strong>de</strong>l consisting <strong>of</strong> reflection codified by knowledge, self-organization with<br />

emerging effects and self-adjustment at the level <strong>of</strong> the mind that link the<br />

information received over the time to the experienced feelings, giving rise to <strong>of</strong>ten<br />

new thoughts and feelings. In terms <strong>of</strong> cognitive sciences, consciousness is the<br />

faculty <strong>of</strong> un<strong>de</strong>rstan<strong>din</strong>g all internal and external phenomena that relate to us.<br />

Accor<strong>din</strong>g to some, conscience is not a moral instance that tells you what is right<br />

and what is wrong, it is not a human attribute but an attribute <strong>of</strong> the intelligence in<br />

our mind (Dennett C. Daniel, 1991). Conscience is related to thought as a specific<br />

human feature. The subject <strong>of</strong> human thought is the entire world surroun<strong>din</strong>g the<br />

man and the man himself, his place in this world, all these lea<strong>din</strong>g to the purpose<br />

<strong>of</strong> his life, whether he realizes it or not. A second characteristic <strong>of</strong> consciousness<br />

is judgment, i.e. the ability to distinguish well from evil. A third feature <strong>of</strong><br />

consciousness is that it triggers man’s will. By will, the man produces facts:<br />

thoughts, words and works (gestures). Without its will, the man cannot act<br />

consciously. These three characteristics <strong>of</strong> consciousness - thought, judgment and<br />

will – but also the emotive states <strong>de</strong>termine entirely man’s attitu<strong>de</strong> towards<br />

himself, towards his fellowmen, towards society. That is way man’s actions show<br />

the quality <strong>of</strong> his consciousness. His consciousness dictates his behavior, his<br />

attitu<strong>de</strong> towards himself, towards his fellowmen, towards his society.<br />

We should make a clear distinction between conscience and consciousness 2 . Being<br />

conscious is un<strong>de</strong>rstood to have a distinct meaning than having a conscience, i.e. to<br />

"hear" that inner voice, which always shows us what is right and what is true. Free<br />

will gives us, unfortunately, the right to overri<strong>de</strong> the advice <strong>of</strong> conscience.<br />

1 Enculturation - process <strong>of</strong> assimilation <strong>of</strong> a certain form <strong>of</strong> culture, by training and education<br />

throughout the life.<br />

2 Consciousness - the fact <strong>of</strong> being aware <strong>of</strong> the surroun<strong>din</strong>g reality, <strong>of</strong> people’s own possibilities,<br />

the obligations that people have in society to achieve the goals set previously.<br />

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Man, Machines and Conscience? 19<br />

Consciousness is a process <strong>of</strong> cognitive reflection over the world and the man<br />

himself. We speak, thus, about world consciousness and self-consciousness. While<br />

world consciousness is coercive, showing the real dimension <strong>of</strong> things, the<br />

unrelenting, objective necessity, self-consciousness is the key condition <strong>of</strong> the selfadjusting<br />

activism, <strong>of</strong> selectivity and creative intervention in the environment. The<br />

world consciousness is based on mo<strong>de</strong>ls or images <strong>of</strong> the objective reality, while<br />

self-consciousness is based on the mo<strong>de</strong>l <strong>of</strong> the self and on personal traits.<br />

Consciousness must be consi<strong>de</strong>red in the first place, in unity with the social<br />

human activity <strong>of</strong> transforming the world, <strong>of</strong> adapting. It forms in time, un<strong>de</strong>r the<br />

influence <strong>of</strong> society, <strong>of</strong> its principles; through family, schools, books, by verbal<br />

exchanges between the individual and those around him, through his thoughts<br />

formed in contact with the evolution environment. Of all the species <strong>of</strong> the earth,<br />

the man is the only one who becomes just like the others provi<strong>de</strong>d that he<br />

<strong>de</strong>velops, evolves in the human society. Man does not become man if he is kept in<br />

isolation 1 from human society (Dulea Gabriel, 2005).<br />

The issue <strong>of</strong> consciousness will lead to an important frontier for mankind as well.<br />

A science <strong>of</strong> consciousness begins to <strong>de</strong>velop and the nature <strong>of</strong> the consciousness<br />

could have significant implications for the society. Man and human<br />

consciousness, with all the scientific and cultural <strong>de</strong>velopments and the religions<br />

that preach what is right and not what is wrong, have failed to create a true<br />

civilization, the social and human civilization 2 . Man might not be able to create a<br />

true civilization because <strong>of</strong> its genes that prevail over its culture. Thierry <strong>de</strong><br />

Montbrial noted: “don’t we have reasons to think that it, the consciousness,<br />

continues to grow if not progress? This is the message <strong>of</strong> great religions. This is<br />

also the message <strong>of</strong> science because it makes us revise continuously our image<br />

about the universe and our place in the universe ...". (Thierry <strong>de</strong> Montbrial, 1999).<br />

A long <strong>de</strong>bated question in philosophy is whether consciousness exists as a brain<br />

specific phenomenon or it is inherent in all matter (principle known as the<br />

principle accor<strong>din</strong>g to which “everything has a conscience”, which can be found<br />

in ancient philosophies).<br />

1 From the literature it is known the case <strong>of</strong> the twins, one <strong>of</strong> which was stolen by the monkeys<br />

(known cases). The other one grew in the city and became a mature man: he graduated a college,<br />

he got a job, he knew to browse the internet etc. The one grew by the monkeys became an animal:<br />

he couldn’t talk, he couldn’t admire a landscape, he couldn’t walk on two feet and used "all fours"<br />

instead (actual cases are known).<br />

2 M. Draganescu claimed in August 2000 within the exhibition <strong>of</strong> “The inevitability <strong>of</strong><br />

globalization and the Information Society” that “By social civilization we must un<strong>de</strong>rstand the<br />

quality <strong>of</strong> the relations between people, between groups, nations, states, ethnic groups, institutions,<br />

and their relations with the natural and artificial-technical environment, all consi<strong>de</strong>red in<br />

connection with human, ethical and aesthetic criteria <strong>of</strong> the manifestation <strong>of</strong> a certain point <strong>of</strong><br />

man’s life in its existence”.<br />

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20 Stefan Iancu<br />

H.S. Green 1 relates the functioning <strong>of</strong> the brain to quantum processes that produce<br />

unpredictable effects. (Green H.S., 2000). A very interesting point <strong>of</strong> Green's<br />

thinking is that intelligence cannot be connected to consciousness. This argument<br />

was confirmed by the artificial intelligence that showed that there can be<br />

intelligence, in a primary, unconsciously form.<br />

Our problem, <strong>of</strong> all <strong>of</strong> us, is the simple fact that, our consciousness is always<br />

subject to thoughts and judgment. We continuously perfect ourselves by simply<br />

un<strong>de</strong>rstan<strong>din</strong>g that, in the or<strong>de</strong>r established by the reason that created us, the<br />

consciousness is superior to thoughts and we have an obligation to live rationally<br />

and therefore responsibly. And the society, to the formation <strong>of</strong> which each <strong>of</strong> us<br />

contributes, will become, in its turn, more responsible, giving, thus, finality to its<br />

becoming.<br />

3. Information processing in the human thinking system<br />

The tenth <strong>de</strong>ca<strong>de</strong> <strong>of</strong> the twentieth century was the brain <strong>de</strong>ca<strong>de</strong>; a period in which<br />

the knowledge acquired about the brain excee<strong>de</strong>d the knowledge acquired in<br />

seven or eight <strong>de</strong>ca<strong>de</strong>s earlier. New discoveries have led to the establishment <strong>of</strong><br />

connections between human performance, failures and diseases, not only with<br />

brain biochemistry but also with genetic factors. One can say without any<br />

exaggeration, that 60% <strong>of</strong> the mental functions are genetically <strong>de</strong>termined. In<br />

other words, genes <strong>de</strong>termine the limits <strong>of</strong> our capacities and the environment<br />

<strong>de</strong>termines how completely this potential is achieved.<br />

The i<strong>de</strong>a <strong>of</strong> a neural network emerged in the '60s <strong>of</strong> the twentieth century and it<br />

was put into practice in the 90s <strong>of</strong> the same century once the neural scanners<br />

appeared. But how can the attention mood are "caught"? The only option available<br />

to the researchers was to catch the precise moment <strong>of</strong> “becoming conscious”, i.e.<br />

when we un<strong>de</strong>rstand a joke or solve a mystery like fin<strong>din</strong>g the difference between<br />

two almost i<strong>de</strong>ntical pictures. Studies on these phenomena have led to a mo<strong>de</strong>l,<br />

wi<strong>de</strong>ly accepted today, namely that <strong>of</strong> “the conscious working space”. Accor<strong>din</strong>g<br />

to this mo<strong>de</strong>l, our neurons are organized into two distinct areas: on the one hand<br />

small brain circuits, a kind <strong>of</strong> “processors” that generate unconscious mental<br />

representations and on the other hand, “a working space” responsible for the<br />

conscious representations. This, “working space” can support only one image at a<br />

time, and therefore each processor that composes it is in competition with the<br />

others to impose its own information. There are several factors that make a<br />

representation to prevail over another. This happens, for example, when we are<br />

focused on a painting but we react instantly if we hear our name pronounced. The<br />

same principle governs the “déjà vu” states. This is the most accepted mo<strong>de</strong>l, but<br />

1 H.S. Green Pr<strong>of</strong>essor <strong>of</strong> Physics at the Univ. <strong>of</strong> A<strong>de</strong>lai<strong>de</strong>, Australia;<br />

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Man, Machines and Conscience? 21<br />

it is far from explaining everything, for instance we do not know, the "language"<br />

through which neurons communicate with each other, neurologists barely perceive<br />

a vague background “noise”.<br />

In 2000, Arvid Carlson, Paul Greengard and Eric R. Kan<strong>de</strong>l received the Nobel<br />

Prize for medicine for their crucial discoveries in un<strong>de</strong>rstan<strong>din</strong>g the normal<br />

functioning <strong>of</strong> the human brain 1 . The study <strong>of</strong> the functional connection between<br />

brain and mind has been done by similarity to computer connection - program,<br />

although it is known that a computer is not a brain, but because computer<br />

programs are <strong>de</strong>signed by people with brain, it has been consi<strong>de</strong>red that a<br />

computer for which these programs are written could represent, based on a<br />

comparison, a mo<strong>de</strong>l in the analysis <strong>of</strong> the connection brain / mind, and the<br />

distinction among brain, mind and human reason has been consi<strong>de</strong>red to be<br />

similar to the distinction between machine (hardware), inferior or s<strong>of</strong>t programs<br />

(for example operating systems) and superior or hard programs 2 . The similarity<br />

between the two distinctions has been based solely on the fact that human reason<br />

and the high level programs are both higher forms <strong>of</strong> organization.<br />

I, personally, believe that, because the nature <strong>of</strong> human reason as a superior form<br />

<strong>of</strong> organization <strong>of</strong> the functional connection between brain and mind is yet<br />

1 The human brain has about 1500 cmc, being about 5 times more massive than the one <strong>of</strong> the<br />

primates <strong>of</strong> the same weight, it represents about 2% <strong>of</strong> body mass, consumes 20% <strong>of</strong> the total<br />

oxygen pumped through the heart arteries and is composed <strong>of</strong> 1,000 billion nerve cells, each nerve<br />

cell forming thousands <strong>of</strong> contact points, the so-called synapses (the contact area between two<br />

neurons), and the communication among nerve cells is ma<strong>de</strong> through chemicals called<br />

neurotransmitters. When a neurotransmitter substance stimulates a nerve cell, its signal is<br />

transmitted through a process called slow synaptic transmission, a process involving an essential<br />

chemical reaction, protein phosphorylation which changes the functioning <strong>of</strong> nerve cells. The<br />

resulted changes may last from seconds to hours. The slow synaptic transmission is the one that<br />

controls both our movements and processes <strong>of</strong> the brain, involved in emotions and reactions to<br />

substances that cause addiction. Human brain reacts to what we see or hear due to the<br />

neurotransmitter substances carrying signals in nerve cells and because memory functions are<br />

achieved through changes in the forms and functions <strong>of</strong> the synapses.<br />

2 Currently, in the literature (M Voicu, 2006) there are two levels <strong>of</strong> artificial intelligence:<br />

inferior or s<strong>of</strong>t level - ensures the <strong>de</strong>velopment <strong>of</strong> non-biological processes that require a<br />

smart management such as the management <strong>of</strong> some production processes, making analysis, the<br />

game <strong>of</strong> chess, processing, un<strong>de</strong>rstan<strong>din</strong>g and natural language synthesis. This level, consi<strong>de</strong>red<br />

inferior, in fact, provi<strong>de</strong>s a more accurate and faster memory than the human one, it has a greater<br />

storage capacity than the human one and it can acquire and provi<strong>de</strong> instant knowledge;<br />

superior or hard level - can give the possibility to the machine to have smart reactions<br />

similar to the human ones if two conditions are met: a computing capacity <strong>of</strong> at least 10 16<br />

operations per second and an artificial intelligence s<strong>of</strong>tware similar to the human one. In 2005,<br />

IBM Blue Gene/L PC already achieved 10 14 operations per second and if estimates are ma<strong>de</strong><br />

accor<strong>din</strong>g to Moore’s law, confirmed by the microelectronics industry, it might reach, in constant<br />

prices, 10 16 operations per second in 2020.<br />

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22 Stefan Iancu<br />

unknown, the comparative study <strong>of</strong> the brain / mind relationship using similar<br />

rules to computer/ computer program may be only the beginning <strong>of</strong> the study<br />

which could be beneficial only to computer science <strong>de</strong>velopment. As research<br />

carried out revealed that there was no apparent connection between the functions<br />

<strong>of</strong> the neural networks that constitute the brain and the functions <strong>of</strong> a computer<br />

system, there should be a thorough concern to i<strong>de</strong>ntify the real nature <strong>of</strong> the<br />

structure <strong>of</strong> human reason as a result <strong>of</strong> a superior form <strong>of</strong> organization <strong>of</strong> the<br />

functional connection between brain and mind.<br />

Although in the past 10-15 years very important steps have ma<strong>de</strong> in the study <strong>of</strong><br />

information processing, it still cannot be said with respect to human thought that it<br />

has been <strong>de</strong>ciphered or that the mechanism <strong>of</strong> thought generating new knowledge<br />

is known. In an article published in 1998 in “The Economic Tribune” (Iancu. St,<br />

1998), I stated that a computing machine that thinks could not be <strong>de</strong>vised because<br />

the mechanism <strong>of</strong> human thinking was not known yet.<br />

If a computer is able to handle a large number <strong>of</strong> “0” and “1”, it is very hard for it<br />

to recognize an object or to read a manuscript, tasks that the brain makes easily.<br />

The efficacy <strong>of</strong> human brain, accor<strong>din</strong>g to an American-Swiss team from the<br />

Institute <strong>of</strong> neuro-science in Zurich, is the result <strong>of</strong> its hybrid character both<br />

binary and analog. There are claims accor<strong>din</strong>g to which the problem <strong>of</strong> <strong>de</strong>signing<br />

artificial intelligence s<strong>of</strong>tware to obtain similar reactions to the human ones can be<br />

solved. The temporal and spatial resolution <strong>of</strong> scanning the human brain<br />

progresses exponentially, so that observations in real-time <strong>of</strong> human neural<br />

networks 1 are already possible. Mathematical mo<strong>de</strong>ls and validated simulations <strong>of</strong><br />

several tens <strong>of</strong> brain regions, inclu<strong>din</strong>g regions <strong>of</strong> the cerebellum, where is the<br />

majority <strong>of</strong> brain neurons, have been <strong>de</strong>veloped. Although the co-operation in<br />

interaction <strong>of</strong> all these mo<strong>de</strong>ls has not been simulated yet, at present, it is<br />

consi<strong>de</strong>red that the conditions necessary to provi<strong>de</strong> solutions for hard intelligence<br />

will be created in approximately two <strong>de</strong>ca<strong>de</strong>s.<br />

Compared with the human brain, the computer presents several advantages in the<br />

sense that if it has the correct s<strong>of</strong>tware, it does not forget and does not do any<br />

mistakes. The human brain has reached a high <strong>de</strong>gree <strong>of</strong> perfection due to its<br />

continuous evolution and adaptation, but it forgets and does errors. Consequently,<br />

the similarity between brain/mind and computer/program is inconsistent. If<br />

thinking is a non-algorithmic process operating primarily with images, the<br />

computer is a rigorously logic algorithmic machine, even when it has to process<br />

erroneous data. If the rules <strong>of</strong> logic are rules <strong>of</strong> correct reasoning, thought<br />

1 In the "Wired" from March 2009 it has been stated that “The center <strong>of</strong> human memory<br />

consi<strong>de</strong>red, not long ago, too chaotic to be <strong>de</strong>co<strong>de</strong>d, might be <strong>de</strong>ciphered soon.” Through some<br />

research conducted at the University College from London the researchers succee<strong>de</strong>d, using the<br />

cerebral activity <strong>of</strong> four subjects in a virtual room, to i<strong>de</strong>ntify the exact place where they were.<br />

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Man, Machines and Conscience? 23<br />

processes, emotions and human feelings are not governed only by rules <strong>of</strong> logic.<br />

Studies have shown that there is no global relationship between brain and mind. It<br />

has been found that several distinct parts <strong>of</strong> the brain may generate separate or<br />

parallel effects in the mental process. Human mind is capable <strong>of</strong> i<strong>de</strong>ntifying a<br />

piece <strong>of</strong> information and a structure known in various forms <strong>of</strong> presentation. For<br />

example, a driver with experience i<strong>de</strong>ntifies if the engine works properly or not by<br />

the noise it makes. A new sound, which he has not heard before, may make him<br />

un<strong>de</strong>rstand that the engine is not working properly (Karl Pribram, 2007).<br />

Let’s see what happens today. Deciphering the human genome (information that<br />

can be stored on 80,000 compact discs) and elucidating the relationships between<br />

genes and their effects may, in the next 10 years, lead to the domination <strong>of</strong> the<br />

society and hopefully <strong>of</strong> the socio-human consciousness, <strong>of</strong> the whole human<br />

biological foundation. Its change, not only for medical purposes, due to a<br />

controlled evolution, a self-controlled evolution actually, that could lead to<br />

characteristics that <strong>de</strong>termine favorable features for a superior conscience and<br />

socio-human civilization.<br />

4. Man-to-man, man-to-machine and machine-to-machine<br />

intercommunication<br />

The main means <strong>of</strong> man-to-man intercommunication 1 is spoken language. Any<br />

human communication has both a <strong>de</strong>sirable and an unpredictable and sometimes<br />

even unwanted effect by the speaker. In interpersonal communication, the mood<br />

and <strong>de</strong>sire <strong>of</strong> the receiver to communicate may have a key role in an efficient<br />

exchange <strong>of</strong> i<strong>de</strong>as and information.<br />

The context <strong>of</strong> the communicative act, its duration and the level <strong>of</strong> knowledge and<br />

intercommunication between speakers, the level <strong>of</strong> knowledge in the area to<br />

which the subject <strong>of</strong> the conversation belongs to, etc. play a significant role in the<br />

person-to-person communication. In current human language we use a large<br />

number <strong>of</strong> metaphors (e.g. "time flies like an arrow") and the problem <strong>of</strong><br />

un<strong>de</strong>rstan<strong>din</strong>g metaphors is related to the problem <strong>of</strong> living, the central problem in<br />

un<strong>de</strong>rstan<strong>din</strong>g the concept <strong>of</strong> consciousness as well (GH von Wright, 1995). A<br />

familiar neighborhood can make us un<strong>de</strong>rstand and control complex phenomena,<br />

living a phenomenon (a situation) being fundamental to its un<strong>de</strong>rstan<strong>din</strong>g.<br />

It has not been possible so far to create a computer program that allows man-tomachine<br />

or machine-to-machine intercommunication in human spoken language,<br />

perfectly i<strong>de</strong>ntical to human dialogue. The problems encountered in a verbal<br />

dialogue with a machine are generated especially by the idiomatic language 2 ,<br />

1 Intercommunication - the mutual conversation between several discussion partners.<br />

2 Idiomatic - all the characteristics <strong>of</strong> a language; relevant to an idiom (a generic term for concepts<br />

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24 Stefan Iancu<br />

which, accor<strong>din</strong>g to some authors are insurmountable in un<strong>de</strong>rstan<strong>din</strong>g the<br />

meanings <strong>of</strong> sentences.<br />

Currently, one <strong>of</strong> the contextual problems found in the dialogue with a machine,<br />

in human language, is the sequence <strong>of</strong> the replies. This issue is treated in Austin 1<br />

and J.R. Searle 2 ’s theory <strong>of</strong> speech acts which places each line from a dialogue in<br />

a well-specified category: information, <strong>de</strong>mand, <strong>of</strong>fer, etc.<br />

Any man-to-machine communication involves an interface ma<strong>de</strong> <strong>of</strong> all the real<br />

physical elements (keyboard, screen, mouse, etc.) or the virtual ones (windows,<br />

menus, other ways <strong>of</strong> display and interaction displayed on the screen) and the<br />

s<strong>of</strong>tware involved in the dialogue between a man and a computer or computer<br />

network. The human factor is <strong>de</strong>cisive in <strong>de</strong>signing and operating such interfaces<br />

(Trausan-Matu Stefan, 2000).<br />

In man-to-machine dialogue, the key effect is given by the information<br />

interaction, the physical interaction between man and machine having only a<br />

secondary role, directed towards the facilitation <strong>of</strong> the information interaction<br />

(pressing some keys, moving the mouse, etc.). Both man and machine (the<br />

electronic computer from the control system) have different representations <strong>of</strong> the<br />

information (the computer - memory bits; in programming languages - symbolic<br />

structures; and the man - symbolic structures and images from the memory). The<br />

machine provi<strong>de</strong>s information to the human discussion partner in a certain form<br />

(alphanumeric, graphic, imaging, auditory, tactile, etc. form) and the latter takes<br />

them, makes certain judgments and as a result, it selects a particular processing<br />

variant and gives certain or<strong>de</strong>rs. All these interactions, subject to some possible<br />

disturbances are intermediated by signs and signals, which turn into ways <strong>of</strong> manto-machine<br />

communication carried out through a communication channel<br />

accor<strong>din</strong>g to a certain co<strong>de</strong>.<br />

People will interact with the computer making it able to respond and give<br />

evi<strong>de</strong>nce <strong>of</strong> un<strong>de</strong>rstan<strong>din</strong>g. Such technology is already experienced in the<br />

laboratory. Verbal communication technology increased by natural language<br />

<strong>of</strong> language, dialect, subdialect or speech).<br />

1 John Langshaw Austin (28 March 1911-8 February 1960) a philosopher <strong>of</strong> the language, who<br />

contributed to the birth <strong>of</strong> this field. He held a very important place in the English philosophy <strong>of</strong><br />

the language alongsi<strong>de</strong> Wittgenstein (Ludwig Josef Johann Wittgenstein-b. 26 April 1889,<br />

Vienna - d. 29 April 1951 - was an Austrian philosopher, author <strong>of</strong> some fundamental<br />

contributions in the <strong>de</strong>velopment <strong>of</strong> mo<strong>de</strong>rn logic and the philosophy <strong>of</strong> the language) for the way<br />

in which they looked at the way words are used (use) and to elucidate the sense (meaning).<br />

2 John Rogers Searle (born 31 July 1932) Pr<strong>of</strong>essor <strong>of</strong> Philosophy at the University <strong>of</strong> California,<br />

Berkeley, known for his contributions to the philosophy <strong>of</strong> language, the philosophy <strong>of</strong> mind and<br />

consciousness, over the characteristics <strong>of</strong> social reality constructed in opposition to the physical<br />

reality and over the practical reason;<br />

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Man, Machines and Conscience? 25<br />

un<strong>de</strong>rstan<strong>din</strong>g makes a computer to un<strong>de</strong>rstand and participate in the interaction.<br />

Let us imagine that in the near future it will be possible to ask a computer to make<br />

all the arrangements necessary for a trip to Sinaia for the weekends. The computer<br />

should un<strong>de</strong>rstand from “his knowledge base” that “we" means our entire family<br />

that our family has certain preferences regar<strong>din</strong>g the means <strong>of</strong> transport, and it<br />

should automatically make reservations on the date and time requested, that the<br />

family has certain accommodation preferences to satisfy by booking early seats,<br />

etc. The computer should contact several travel agents and negotiate, select and<br />

<strong>de</strong>mand a particular journey in preferential conditions to the agency which<br />

ensures the highest performance/cost ratio. Thus, it will take several seconds to<br />

launch the request to the computer and half a day nee<strong>de</strong>d to negotiate with travel<br />

agencies will be spared.<br />

"Intelligence" implies the possibility <strong>of</strong> connecting autonomous <strong>de</strong>vices in a<br />

network that will then work together. Let us imagine that a company which runs<br />

the operation <strong>of</strong> 800 blocks <strong>of</strong> housing for rent from a distance could un<strong>de</strong>rstand<br />

the behavior <strong>of</strong> the tenants based on the pheromones 1 <strong>of</strong> the occupants. Let us<br />

imagine a piece <strong>of</strong> furniture that could respond to the wishes <strong>of</strong> its user or to<br />

systems that could control the operation <strong>of</strong> a vehicle and could drive it on the<br />

highway 2 .<br />

The researchers from IBM Israel started in 2008 the "Hermes" program that will<br />

create a <strong>de</strong>vice to help the el<strong>de</strong>rly have a computer-assisted memory. The el<strong>de</strong>rly<br />

will be equipped with microphones and miniature vi<strong>de</strong>o equipment to record, at<br />

their command, what they have said, what they have done, where there have been at<br />

a certain time. All this information will be stored and processed to provi<strong>de</strong>, upon<br />

request, electronic "memories" to those with memory slips. The computer will free<br />

man from its daily tasks, giving it the necessary time for creative activities, for<br />

personal, family concerns, etc. What is fiction today will become reality in the next<br />

<strong>de</strong>ca<strong>de</strong> <strong>of</strong> the 21 st century. Will we entrust the logic, daily, algorithmically activity<br />

to the computer as it happened at the beginning <strong>of</strong> the first industrial revolution,<br />

when muscular strength was replaced by the strong arm <strong>of</strong> machines?<br />

As <strong>of</strong> 2000, accor<strong>din</strong>g to the literature, the research direction with the greatest<br />

potential for the <strong>de</strong>velopment <strong>of</strong> information technology is represented by<br />

1 Pheromones - chemical, biologically active substance secreted by the individuals belonging to<br />

different species that influence the process <strong>of</strong> <strong>de</strong>velopment and the behavior <strong>of</strong> other individuals <strong>of</strong><br />

that species or <strong>of</strong> other species.<br />

2 The future belongs to the intelligent automobiles with reflexes that are faster than the human<br />

ones. In 2008 the license <strong>of</strong> the only road safety system, called Mobileye, was sold in Europe by<br />

two teachers from Israel. It integrates the alarm for danger <strong>of</strong> collision with the one signaling<br />

leaving the road and with the dangerous proximity alarm. The traffic security system is already<br />

installed on luxury cars like BMW, Volvo, Buick and Cadillac.<br />

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26 Stefan Iancu<br />

computers operating autonomously, i.e. computers able to solve their own<br />

operation problems, able to self-repair and become functional again. The term,<br />

"autonomous computer" may sound esoteric but it will have practical<br />

implications, reducing the total cost <strong>of</strong> operation (the cost <strong>of</strong> installation,<br />

operation maintenance, current and periodic maintenance <strong>of</strong> the system) and<br />

eliminating hazards generated by viruses.<br />

Currently, the evolutionist artificial intelligence systems, inspired by biology, as<br />

well as those on artificial life, are increasingly powerful. If most <strong>of</strong> the previous<br />

approaches <strong>of</strong> the artificial intelligence sought to imitate intelligent human<br />

behavior, the solutions provi<strong>de</strong>d by the artificial life sub-domain aim to summarize<br />

some artificial life forms to mo<strong>de</strong>l it as it might be or become, to try to un<strong>de</strong>rstand<br />

the life we are living. The distinction between machine and live nature has not been<br />

<strong>de</strong>termined by the nature <strong>of</strong> the existing machinery. On the contrary, the concepts <strong>of</strong><br />

mind and machine <strong>de</strong>pend one on the other, being in a continuous dialectics.<br />

The problems with the industrial robots and the current automated production<br />

sectors are simpler than those <strong>of</strong> the human-type robot, but they are much more<br />

complex than those <strong>of</strong> the mechanical duck 1 or those <strong>of</strong> the means <strong>of</strong> production<br />

without electronic control and adjustment. Only after the man had had the<br />

electronic means to build the artificial intelligence did it become a characteristic<br />

<strong>of</strong> the automated means <strong>of</strong> production. The law <strong>of</strong> the complementarily between<br />

the mechanical motion and the electronic intelligence marked the technological<br />

<strong>de</strong>velopment in the second half <strong>of</strong> the twentieth century, lea<strong>din</strong>g to the evolution<br />

<strong>of</strong> production machinery and machinery in general. The evolution from the simple<br />

tool to the tool with artificial intelligence ma<strong>de</strong> the world familiar to quantitative<br />

growths, but also important qualitative leaps.<br />

Currently, practical information and communication technology applications,<br />

even wireless, operate separately, in<strong>de</strong>pen<strong>de</strong>nt <strong>of</strong> one another. Machine-tomachine<br />

communication, although in incipient <strong>de</strong>velopment phase is in a<br />

continuous expansion. At present, there is no infrastructure <strong>de</strong>signed to allow a<br />

general intercommunication between telecommunication <strong>de</strong>vices, integrated in<br />

machines equipped with artificial intelligence.<br />

In literature (Kallio Johanna, 2009) it has been estimated that in 2010 the number<br />

<strong>of</strong> the communication <strong>de</strong>vices, integrated in machines equipped with artificial<br />

1 In the winter <strong>of</strong> 1738-1739, Jacques <strong>de</strong> Vaucanson (1709-1782, French engineer) built and ma<strong>de</strong><br />

a <strong>de</strong>monstration in Paris with a mechanical duck, consi<strong>de</strong>red to be the first robot that was able to<br />

peck grains that after a reasonable time, necessary for “digestion”, were eliminated. Besi<strong>de</strong>s this<br />

mechanical duck, during the same <strong>de</strong>monstration two other mechanical constructions representing<br />

a flutist and a tambourine drummer and whistle singer were presented. In addition to the<br />

commercial, philosophical, popular and pr<strong>of</strong>essional success, the three presented automatic<br />

<strong>de</strong>vices impressed Voltaire, who called Vaucanson, “a rival to Prometheus”.<br />

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Man, Machines and Conscience? 27<br />

intelligence will be 1,000 times larger than the number <strong>of</strong> the mobile phones,<br />

which currently exceeds one billion. When all the existing communication <strong>de</strong>vices<br />

will be interconnected to the Internet, new opportunities for machine-to-machine<br />

intercommunication will appear. Usenet project (Ubiquitous M2M Service<br />

Network 1 ) launched by Eureka/ITEA 2, in 2008 aimed to solve this<br />

interoperability problem within three years, provi<strong>din</strong>g information collection,<br />

transmission and processing services and creating an interactive system with<br />

machines equipped with telecommunication <strong>de</strong>vices.<br />

Ubiquitous M2M Service Network will provi<strong>de</strong> opportunities and benefits that are<br />

essential for the activities <strong>of</strong> various companies, in particular if the systems that<br />

control their key processes are able to use real-time information, generated by the<br />

machine-to-machine (M2M) intercommunication. The main result <strong>of</strong> the M2M<br />

system operation will be that all the interconnected companies will be able to<br />

increase their service quality, to reduce cost prices and increase customer<br />

satisfaction.<br />

5. Can machines have a conscience?<br />

Currently there are many machines, whose “behavior” suggests that they are<br />

endowed with mental processes. For example, the aircrafts equipped with<br />

autopilot can fly by themselves on air routes: they respond to external “sensorial”<br />

information; they “take <strong>de</strong>cisions” on the flight; they communicate with other<br />

aircrafts; they “know” when they “need” fuel; they “feel” a potential danger, etc.<br />

The way in which an autopilot functions restores the following question: Are<br />

humans the only ones who make <strong>de</strong>cisions, who communicate? Machines do not?<br />

And, yet, the problem is not really that simple. For a number <strong>of</strong> cognitive<br />

researchers, strong artificial intelligence is not just a tool for formulating and<br />

testing hypotheses concerning the human world, but also – if it is well-planned – a<br />

mind that seems to un<strong>de</strong>rstand and have other cognitive processes as well, in<br />

brief, a conscious mind. John Rogers Searle thought that it was impossible for<br />

machines (even with strong artificial intelligence) to have a consciousness. He<br />

consi<strong>de</strong>red that there is only one “machine” ma<strong>de</strong> <strong>of</strong> flesh and blood or<br />

neuroproteins that may be conscious, the phenomenon <strong>of</strong> consciousness being<br />

inaccessible to silicon and metal.<br />

In the SF literature, the existence <strong>of</strong> robots with self-consciousness and <strong>de</strong>cisionmaking<br />

capacity as a result <strong>of</strong> their own judgments in accordance with the social<br />

requirements 2 has been imagined since the first <strong>de</strong>ca<strong>de</strong>s <strong>of</strong> the twentieth century.<br />

1 M2M - machine/two/to machine.<br />

2 In 1921 Karel Capek’s “Rossum’s Universal Robots” was published. It is about the construction<br />

by people <strong>of</strong> better robots that were sent to fight in wars. Robots <strong>de</strong>ci<strong>de</strong> that fighting in a war is<br />

madness and they conquer the world to dominate peace.<br />

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28 Stefan Iancu<br />

If we consi<strong>de</strong>r the elements <strong>of</strong> intelligence based on a more or less <strong>de</strong>veloped<br />

nervous system, <strong>of</strong> so many creatures inferior to man, all machines with all their<br />

automated perfection, inclu<strong>din</strong>g with microelectronic or nanoelectronic structures<br />

<strong>of</strong> control and adjustment, seem primitive to us compared with the simplest<br />

creatures and with the latest machines equipped with artificial intelligence. "The<br />

simplest living cell is so complex that supercomputer mo<strong>de</strong>ls may never simulate<br />

its behavior" (Wayt Gibbs W., 2001).<br />

Some say that mankind will never build a machine with a conscience. It is in<strong>de</strong>ed<br />

difficult to imagine how a brain-robot could be the support <strong>of</strong> a conscience. But at<br />

the same time it is difficult to imagine the way in which our organic brain may be<br />

the seat <strong>of</strong> a conscience. And yet we accept it easily even though we do not imagine<br />

how it could be possible. The genetic revolution <strong>of</strong> the ’60s <strong>of</strong> the last century has<br />

ma<strong>de</strong> the hopes <strong>of</strong> buil<strong>din</strong>g a conscious machine revive. It is argued in the literature<br />

(Vinge Vernor, 2008) that mankind became efficient enough to be consi<strong>de</strong>red a<br />

superhuman being through its computer networks and the created databases.<br />

Globalization, increased today by the Internet, is accompanied by the creation <strong>of</strong> a<br />

global network which is assumed to become a network <strong>of</strong> artificial intelligence and<br />

in the future with conscious no<strong>de</strong>s <strong>of</strong> artificial intelligence. What kind <strong>of</strong> conscience<br />

will such a network have? Green thinks that there will be a symbiosis <strong>of</strong> human<br />

conscience with this conscience <strong>of</strong> the Internet by creating an ecological system that<br />

will lead to a great intelligence 1 and wisdom (Green H.S., 2000).<br />

The artificial intelligence 2 is a discipline that provi<strong>de</strong>s methods, techniques and<br />

information tools, based on specific ways <strong>of</strong> information processing, which<br />

mimics different facets <strong>of</strong> complex problem solving, which could not be<br />

satisfactorily resolved only by using numerical methods. Artificial intelligence is<br />

the result <strong>of</strong> combining computer science, physiology and philosophy (logic),<br />

cognitive psychology and management science, biology. Research in automatic<br />

In 1950, Isaac Asimov published the work “I, Robot” in which he set out the three fundamental<br />

laws <strong>of</strong> robotics:<br />

a. - A robot may not injure a human being, or, through inaction, allow a human being to come to<br />

harm.<br />

b. - A robot must obey the or<strong>de</strong>rs given it by human beings, except where such or<strong>de</strong>rs would<br />

conflict with the First Law.<br />

c. - A robot must protect its own existence, except where such protection would conflict with the<br />

First or Second Law.<br />

1 Intelligence - the capacity <strong>of</strong> the individual to adapt to new circumstances, to <strong>de</strong>termine the<br />

essential relations and to find a way out <strong>of</strong> a given situation, to solve new problems.<br />

2 Artificial intelligence - the capacity <strong>of</strong> advanced technical systems to achieve performance that<br />

could be i<strong>de</strong>ntical to those <strong>of</strong> humans. The term indicates a concept (in the wi<strong>de</strong> sense advocated<br />

by Turing’s test), an area (a branch <strong>of</strong> information technology that <strong>de</strong>als with intelligent behavior<br />

automation) and an instrument (for the <strong>de</strong>velopment <strong>of</strong> applications, objects and intelligent<br />

technologies).<br />

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Man, Machines and Conscience? 29<br />

learning, automatic processing <strong>of</strong> natural language, sensorial perception, ma<strong>de</strong> it<br />

possible for <strong>scientists</strong> to build machines that perceive and un<strong>de</strong>rstand, leaving the<br />

impression that they reason.<br />

Perhaps the best way to assess whether a machine has intelligence is the one<br />

shown by Alan Turing 1 . He said that "a computer <strong>de</strong>serves to be consi<strong>de</strong>red<br />

intelligent if it makes the man to believe that its actions with such a computer are<br />

its actions with another man" - (http://library.thinkquest.org/2705/basics.html).<br />

The issue <strong>of</strong> artificial intelligence has been <strong>de</strong>fined on the one hand, in<br />

comparison with the ability to reason, and on the other hand, in relation to<br />

behavior skills. Basically, artificial intelligence involves both a better<br />

un<strong>de</strong>rstan<strong>din</strong>g <strong>of</strong> human thinking and a rational way <strong>of</strong> action. “Rationalism and<br />

the human factor <strong>de</strong>fine the four major categories <strong>of</strong> <strong>de</strong>finitions: systems that<br />

think like humans, systems that think rationally, systems that act like humans,<br />

systems that act rationally. The rational-human dichotomy does not imply that<br />

people are irrational, but that people <strong>of</strong>ten make (sometimes explainable) mistakes<br />

"(Elena Solunca Moise, 2002).<br />

Artificial intelligence involves the storage and the logic processing <strong>of</strong> a very large<br />

volume <strong>of</strong> data and symbols with very high speeds. Therefore its support is the<br />

static electronic memories <strong>of</strong> high capacity in small physical volume and the<br />

logical drives that have taken the form <strong>of</strong> microprocessors. The evolution <strong>of</strong> the<br />

artificial intelligence is closely linked to micro and nanotechnology <strong>de</strong>velopments<br />

in general and the <strong>de</strong>velopment <strong>of</strong> computer science in particular, significant<br />

results being achieved in recent <strong>de</strong>ca<strong>de</strong>s, both in the conceptual and the applied<br />

plans, as a result <strong>of</strong> introducing the electronic circuits in the structure <strong>of</strong> <strong>de</strong>vices,<br />

machines, facilities and <strong>de</strong>velopment <strong>of</strong> operating systems in real time (Iancu St.,<br />

2003).<br />

Human brain has been consi<strong>de</strong>red a supercomputer, which might interact with<br />

or<strong>din</strong>ary computers. It is also thought that, in the future, the print <strong>of</strong> a man’s<br />

consciousness could be stored on a computing support, ensuring thus the<br />

immortality <strong>of</strong> the individual. Accor<strong>din</strong>g to the literature (Koch Christ<strong>of</strong>, 2008) in<br />

the next 25 years it will be possible for a person to “transfer” its mind, memory,<br />

intelligence, its entire personality to a machine and thus this machine could<br />

acquire consciousness 2 .<br />

1 Alan Turing (1912 - 1954), English mathematician, a pioneer in the <strong>de</strong>velopment <strong>of</strong> computer<br />

logic, as it is known at present.<br />

2 Accor<strong>din</strong>g to the literature, clinical studies have shown certain neural activities that <strong>of</strong>fered the<br />

possibility <strong>of</strong> some rudimentary un<strong>de</strong>rstan<strong>din</strong>g <strong>of</strong> billions <strong>of</strong> processes that might constitute the<br />

basis <strong>of</strong> forming a conscience. At the same time it was found that many processes in the brain have<br />

nothing in common with the conscience. Extensive <strong>de</strong>struction <strong>of</strong> cerebellum (the small brain, part<br />

<strong>of</strong> the encephalon located in the rear and bottom <strong>of</strong> the head) does not affect a person's conscience,<br />

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30 Stefan Iancu<br />

If a person’s mind, memory, intelligence could be reduced to the level <strong>of</strong> a<br />

structure <strong>of</strong> electrons, it will become possible for this structure to be copied and<br />

multiplied, sold, pirated and/or, "<strong>de</strong>leted" from the memory <strong>of</strong> the machine. Such<br />

a structure could also be unified with another electronic structure with artificial<br />

intelligence, improving the operating parameters <strong>of</strong> the latter. For the moment,<br />

such statements are and will be only some SF scenarios because as long as no one<br />

knows how the human brain works, it is impossible to know what a conscience is.<br />

Hans Moravec 1 thinks that the intelligence <strong>of</strong> robots, even before 2050, will<br />

exceed by far the intelligence <strong>of</strong> people (Hans Moravec, 1999). Follower <strong>of</strong> the<br />

principle “Structural science is sufficient to explain the whole nature, inclu<strong>din</strong>g<br />

life, mind and conscience", although he has some doubts on this principle,<br />

Moravec believes that the mere increase in the computing power and memory <strong>of</strong><br />

computers will lead to consciousness without any special precautions in or<strong>de</strong>r to<br />

produce qualia. This is however exclu<strong>de</strong>d by the principle “Structural science is<br />

insufficient and incomplete to explain the whole existence, inclu<strong>din</strong>g life, mind<br />

and conscience", (Draganescu Mihai, 1997 A), principle that also states the need<br />

for the recognition <strong>of</strong> some new physical and information ingredients, <strong>of</strong> a new<br />

physics, <strong>of</strong> some new scientific principles. However, Moravec’s following<br />

statement is very interesting: “In that case, mass-produced, fully educated robot<br />

<strong>scientists</strong> working diligently, cheaply, rapidly and increasingly effectively will<br />

ensure that most <strong>of</strong> what science knows in 2050 will have been discovered by our<br />

artificial progeny!” (Hans Moravec, 1999). It is possible that such robots, let’s call<br />

them quantico-phenomenological ingredients, will appear. Will they be sociohuman?<br />

Or will they take on their own the evolution <strong>of</strong> the conscience on the<br />

Earth and in the Universe? Green believes that the <strong>de</strong>velopment <strong>of</strong> quantum<br />

computers with conscience and that will reproduce themselves will be the next<br />

step in evolution.<br />

All the optimistic forecasts do not state the strict requirements for a machine to<br />

have a conscience. We assume that a machine with conscience does not need<br />

anything more than what humans have. But which are the essential properties <strong>of</strong><br />

human conscience, without which it could not exist? The answer to this question<br />

may refer to the amount <strong>of</strong> integrated information that a human being or a<br />

machine could generate. The man and the machine perceive and become<br />

conscious <strong>of</strong> an existing state separately. For example, a man and a photoelectric<br />

cell 2 can signal if a nearby screen is bright or dark. But while the man by looking<br />

at the light or dark screen perceives a lot <strong>of</strong> information the photodio<strong>de</strong> does not<br />

although there are more neurons in the cerebellum than in any other part <strong>of</strong> the brain.<br />

1 Hans Moravec - Pr<strong>of</strong>essor at Carnegie Mellon University, USA, who has been working for 45<br />

years in the field <strong>of</strong> Robotics.<br />

2 Photoelectric cell – dio<strong>de</strong> whose operation <strong>de</strong>pends on the intensity <strong>of</strong> light flow that falls on it.<br />

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Man, Machines and Conscience? 31<br />

see anything, but it only responds to the presence <strong>of</strong> the luminous flow. The way<br />

in which the man and the photoelectric cell react to the existence <strong>of</strong> light is<br />

distinguished by the amount <strong>of</strong> generated information 1 . When the photoelectric<br />

cell receives the luminous signal it enters one <strong>of</strong> two possible states, while the<br />

man when he sees the dark screen enters a large number <strong>of</strong> possible states. If he<br />

sees black it means he does not see blue, red, green, etc. For the man, the black<br />

screen does not signify only the absence <strong>of</strong> light, but also it could mean the lack<br />

<strong>of</strong> some previously seen and appreciated images. Therefore being conscious<br />

implies being an entity with a huge repertoire <strong>of</strong> states and the level <strong>of</strong> conscience<br />

is given by the quantity <strong>of</strong> integrated information which may be generated.<br />

Therefore humans have a much bigger level <strong>of</strong> consciousness than any machine.<br />

The integrated information theory (IIT) established in science and mathematics<br />

can <strong>de</strong>termine the amount <strong>of</strong> information generated by the integrated systems<br />

consisting <strong>of</strong> several integral parts.<br />

IIT suggests a way <strong>of</strong> assessing the conscience <strong>of</strong> a machine through a kind <strong>of</strong><br />

Turing test for consciousness, and in this sense, Koch Christ<strong>of</strong> and Giulio Tononi<br />

(Koch Christ<strong>of</strong>, 2008) have proposed a version <strong>of</strong> the Turing test in which a<br />

certain scene is presented to the computer and it has to <strong>de</strong>duct the "joke", the<br />

essence <strong>of</strong> the scene, which is perfectly possible for the human judgment (Vinge<br />

Vernor, 2008).<br />

Other attempts to measure the consciousness or the intelligence <strong>of</strong> a machine<br />

failed. Conversations in natural language or participating in strategic games,<br />

consi<strong>de</strong>red human attributes have been performed by computers. Deep Blue<br />

super-computer that <strong>de</strong>feated Garry Kasparov at chess in 1997, discussions with<br />

the computer in natural language on different areas or participating in strategic<br />

games have shown that machines may exceed human performance in narrow<br />

areas, but none <strong>of</strong> these experiences did not reveal the existence <strong>of</strong> a conscience in<br />

a machine.<br />

Accor<strong>din</strong>g to IIT, consciousness implies a large glossary <strong>of</strong> states for a single<br />

integrated system. To be useful, these internal states should be able to provi<strong>de</strong><br />

much information about the world in general. A test used to prove that a machine<br />

has a conscience is whether it can or cannot <strong>de</strong>scribe a scene seen for the first time<br />

and which is different from the huge number <strong>of</strong> scenes stored in its database. A<br />

man, for example, can <strong>de</strong>scribe successfully and in a different manner what<br />

happens in a scene from a photograph, a painting or a scene from a film, seen for<br />

the first time. For a machine equipped with artificial intelligence to un<strong>de</strong>rstand a<br />

picture that it has not seen before or an image that inclu<strong>de</strong>s elements which do not<br />

1 The amount <strong>of</strong> information is measured by reducing the uncertainty that appears when you have<br />

to choose between several possible occurrences.<br />

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32 Stefan Iancu<br />

exist in its database it is still impossible. It will be possible to write a computer<br />

program which will i<strong>de</strong>ntify the objects from a new image based on the multitu<strong>de</strong><br />

<strong>of</strong> objects from its database, but this program does not imply the existence <strong>of</strong> a<br />

conscience. As long as it will not have a huge storage capacity and the computer<br />

program will not be <strong>de</strong>signed to conclu<strong>de</strong> from a multitu<strong>de</strong> <strong>of</strong> possible<br />

combinations in action the items or all the items <strong>of</strong> any potential future image in<br />

different contexts (the picture <strong>of</strong> a child in a gar<strong>de</strong>n with a toy gun in his hand is<br />

completely different than a young man with a gun in his hand at the door <strong>of</strong> a<br />

bank) it will be impossible to speak about the conscience <strong>of</strong> a machine.<br />

In 1986 researchers tried to <strong>de</strong>sign the mo<strong>de</strong>l <strong>of</strong> an artificial brain 1 with 6,000<br />

synapses, using an electronic microscope. Two <strong>de</strong>ca<strong>de</strong>s later, they were still<br />

working at the functional mo<strong>de</strong>l <strong>of</strong> this minimal nervous system. Giorgio Buttazo<br />

showed that G.S. Paul and E. Cox (1996), Ray Kurzweil (1999), Hans Moravec<br />

(1999, 2000) had estimated how complex the human brain was based on the<br />

enormous number <strong>of</strong> synapses (10 12 neurons, each on average with 10 3 synaptic<br />

connections with other neurons, so a total <strong>of</strong> 10 15 synapses). Simulating the human<br />

brain with artificial neural networks taking into account that each synapse requires 4<br />

bytes <strong>of</strong> memory in a computer it results that it would be necessary a memory <strong>of</strong> 4<br />

million Gbytes. Giorgio Buttazo, based on the <strong>de</strong>velopments and trends in the<br />

evolution <strong>of</strong> computers, believes that such a memory can be obtained in 2029<br />

(Buttazo Giorgio, 2001). Note, however, that such a memory is only one <strong>of</strong> the<br />

conditions necessary for a simulation <strong>of</strong> a giant neural mo<strong>de</strong>l and assuming that we<br />

will have <strong>de</strong>termined how consciousness forms with the huge number <strong>of</strong> parameters<br />

whose values are only vaguely suspected, and therefore, I, personally, consi<strong>de</strong>r that<br />

such a simulation is very unlikely to happen in the foreseeable future.<br />

In the literature (Wada Yasuo, 2001) it is stated that the <strong>de</strong>velopment <strong>of</strong><br />

nanotechnologies based on molecular nanoelectronics and quantum <strong>de</strong>vices will<br />

enable the replacement <strong>of</strong> the silicon MOS technology in 2015. The issue <strong>of</strong> brain<br />

knowledge cannot be solved only by improving computer technology while a<br />

theory <strong>of</strong> the mind and consciousness based only on structures and structural<br />

fundamental forces <strong>of</strong> nature is not possible. The phenomenological processes and<br />

the phenomenological reality are equally important for obtaining such a theory<br />

(Drăgănescu Mihai, 2007).<br />

If the structure and the operating mo<strong>de</strong> <strong>of</strong> the human brain are un<strong>de</strong>rstood then we<br />

might un<strong>de</strong>rstand the way in which human consciousness is formed. But this issue<br />

1 Research carried out revealed that there is a category <strong>of</strong> rules which coor<strong>din</strong>ate the activity <strong>of</strong> the<br />

classic systems (e.g. the electronic computer) that can be <strong>de</strong>scribed in Euclidian and/or Newtonian<br />

terms or drafted in Cartesian space/time coor<strong>din</strong>ates and another class <strong>of</strong> rules for the coor<strong>din</strong>ation<br />

<strong>of</strong> the classes <strong>of</strong> systems with fine-grain structure (e.g. the brain), knowing that in the latter may<br />

occur radical changes within the creation process through successive transformations.<br />

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Man, Machines and Conscience? 33<br />

is unlikely to be solved in the 21 st century. If in the literature (Drăgănescu Mihai,<br />

2007) it is stated that the current biological man cannot build a society <strong>of</strong> the<br />

consciousness but only a society <strong>of</strong> predicting the society <strong>of</strong> consciousness, how<br />

can we hope to build a machine with a conscience? Firstly, it would be necessary<br />

for the current biological man and the existing social consciousness to evolve.<br />

Humanity was not able to ensure the management <strong>of</strong> the natural environment <strong>of</strong><br />

our planet. While many natural species are <strong>de</strong>stroyed, different biotechnologies<br />

multiply transgenic plants and animals. How far will this process go? Will<br />

everything that has been <strong>de</strong>signed over millions <strong>of</strong> years in the natural<br />

environment disappear and will we be surroun<strong>de</strong>d only by robots?<br />

Research and the practical implementation <strong>of</strong> the new scientific discoveries and<br />

new technologies should not be fighting against the created natural world, but<br />

only against the motions and the energies <strong>of</strong> the powers <strong>of</strong> the world which are<br />

unnatural and hostile to the natural environment.<br />

6. Conclusions<br />

(1) The consciousness that we have today is the result <strong>of</strong> the ongoing interaction<br />

between tool (i.e. the hand), thought (i.e. the brain/mind), communication (i.e.<br />

the society) and the increasing cultural <strong>de</strong>velopment <strong>of</strong> the individual over<br />

millions <strong>of</strong> years, so it is clearly different from the self-consciousness <strong>of</strong> some<br />

animals endowed with some form <strong>of</strong> intelligence. It is clear that the human<br />

consciousness is part <strong>of</strong> the natural world and that it has contributed to reducing<br />

human progress in favor <strong>of</strong> the human cultural evolution.<br />

(2) Nowadays there are machines which have the ability to un<strong>de</strong>rstand human<br />

language in a particular domain, to read texts written in human language, to<br />

recognize shapes and to process images, there are machines which communicate<br />

among themselves, changing and enriching their databases. However, it is not<br />

known if there are programs that make a machine self-conscious. There are<br />

programs that allow a machine to i<strong>de</strong>ntify the space in which it is placed and<br />

which route to follow to get to another spatial location. It has not been created<br />

the program that could ensure the auto-orientation <strong>of</strong> a machine so that it could<br />

move in a totally unknown space or in a known and easily modified space.<br />

(3) The <strong>de</strong>velopments in science and information technology are taken into<br />

account in the un<strong>de</strong>rstan<strong>din</strong>g <strong>of</strong> the way in which our brain and mind work.<br />

Many conclusions on the possible functioning <strong>of</strong> the brain were drawn by<br />

similarity based on what is known on the functioning <strong>of</strong> the electronic computer.<br />

The possibility <strong>of</strong> higher levels <strong>of</strong> structural organization <strong>of</strong> quantum<br />

information processing in the brain, levels that are to be i<strong>de</strong>ntified by future<br />

research, should be taken into account as well.<br />

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34 Stefan Iancu<br />

(4) Currently, it is not known whether human consciousness <strong>de</strong>pends only on the<br />

scientific laws, still imperfectly known, or if it has been formed as a result <strong>of</strong> the<br />

action <strong>of</strong> the still unknown energy fields. Only after having un<strong>de</strong>rstood the<br />

entire system <strong>of</strong> quantum information processing in the brain will it be possible<br />

to say if machines can be endowed with a conscience or not. These facts lead us<br />

to the conclusion that at present there is no premise to make us believe that the<br />

construction <strong>of</strong> conscious machines, similar to the human one would be possible<br />

in the near future.<br />

(5) What distinguishes humans from the other species is the fact that it is the<br />

only one who affected the natural environment. Human intelligence has<br />

completely <strong>de</strong>ciphered the genome <strong>of</strong> its species. Cloning is already possible, a<br />

scenario <strong>of</strong> a supposed Bing Bang moment has been created, the solar system is<br />

being explored, but man fails to explore and know its own planet, to reveal its<br />

genesis and <strong>de</strong>stiny in the universe. In this context, claiming that the creation <strong>of</strong><br />

a machine with a conscience is a certainty is not consistent with reality. Perhaps<br />

the best answer is that it will NOT be possible to build machines with human<br />

intelligence in the future, but only machines with an algorithmic, binary<br />

intelligence.<br />

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Man, Machines and Conscience? 35<br />

R E F E R E N C E S<br />

[1] *** An Introduction to Artificial Intelligence, http://library.thinkquest.org/2705/basics.html.<br />

[2] Bergson H., Oeuvres, Presses Universitaire <strong>de</strong> France, 1959.<br />

[3] Buttazo Giorgio, Artificial Consciousness: Utopia or real Possibility?, Computer (IEEE),<br />

July 2001.<br />

[4] Brooks Rodney, I, Rodney Brooks, Am a Robot, IEEE Spectrum, June 2008.<br />

[5] Dennett C. Daniel Consciousness Explained, Editura Little, Brown and Company, 1991.<br />

[6] Drăgănescu Mihai, ,On the structural-phenomenological theories <strong>of</strong> consciousness, The<br />

Noetic Journal, 1, No.1, 1997.<br />

[7] Drăgănescu Mihai, De la filos<strong>of</strong>ia mentalului la stiinta mentalului, Revista <strong>de</strong> filos<strong>of</strong>ie,<br />

XLIV, Nr. 5, sept-oct 1997.<br />

[8] Drăgănescu Mihai, On the notions <strong>of</strong> un<strong>de</strong>rstan<strong>din</strong>g and intelligence, NOESIS, XXIII,<br />

1998.<br />

[9] Drăgănescu Mihai, Structural-Phenomenological Theories in Europe and USA, The Noetic<br />

Journal, Vol.2, 1999, No.1-2.<br />

[10] Drăgănescu Mihai, The Frontiers <strong>of</strong> Science and Self-organization, Comunicare la a IV-a<br />

Conferință Mo<strong>de</strong>larea structural-fenomenologică, <strong>Aca<strong>de</strong>mia</strong> Română, București, 20-21 iunie 2000.<br />

[11] Drăgănescu Mihai, Societatea Conştiinţei, Editată <strong>de</strong> Institutul <strong>de</strong> Cercetări pentru<br />

Inteligenţă Artificială al Aca<strong>de</strong>miei Române, Bucureşti, 2007.<br />

[12] Descartes Rene, Oeuvres et letters, Paris, Gallimard, 1953.<br />

[13] Dulea Gabriel, Componenta energetică a psihicului uman: perspectivă psih<strong>of</strong>ilos<strong>of</strong>ică,<br />

Editura Universităţii Naţionale <strong>de</strong> Apărarare, Bucureşti, 2005.<br />

[14] Green H.S., Information Theory and Quantum Physics, Physical foundations for<br />

Un<strong>de</strong>rstan<strong>din</strong>g the Conscious Process, Springer Verlag, Berlin-Hei<strong>de</strong>lberg, 2000.<br />

[15] http://www.acunu.org/millenium/s<strong>of</strong>2006.html.<br />

[16] Iancu Şt, Un calculator electronic nu poate gândi?, Tribuna economică nr. 44/1998.<br />

[17] Iancu Şt, De la sisteme automate la sisteme inteligente, Inventica şi economie nr. 2/2003.<br />

[18] Iancu Şt, Ingineria <strong>de</strong> la roată la inteligenţă artificială, Iaşi, Editura Performantica, 2007.<br />

[19] Kallio Johanna and Latvakoski Juhani „Ubiquitous Machine-to-Machine Service Networks,<br />

„European Research Consortium for Informatics and Mathematics (Ercim) News 76, January,<br />

2009.<br />

[20] Koch Christ<strong>of</strong> and Giulio Tononi, Can Machines Be Conscious, IEEE Spectrum, June 2008.<br />

[21] Laffite J., Reflexions sur la science <strong>de</strong>s machines, Paris, 1932.<br />

[22] La Mettrie, Omul maşină şi alte opere filos<strong>of</strong>ice, Bucureşti, Editura Politică, 1961,<br />

Bucureşti.<br />

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36 Stefan Iancu<br />

[23] Luger G.F. & Stubblefield W.A., Artificial Intelligence and the Design <strong>of</strong> Expert Systems,<br />

2 nd Edition, The Benjamin/Cummings Publishing Company, Inc. Redwood City, CA, 1993.<br />

[24] Moravec Hans, Rise <strong>of</strong> the Robots, Scientific American, <strong>de</strong>cembrie 1999.<br />

[25] Pribram Karl, Quantum Information Processing in Brain Systems and The Spiritual Nature<br />

<strong>of</strong> Mankind, The Center for Frontier Sciences, Special 20 th Anniversary Edition. Volume 16,<br />

Number 1, 2007.<br />

[26] Solunca Moise Elena, Interviu cu Dan Tufiş, M.C. al Aca<strong>de</strong>miei Române, Revista<br />

Aca<strong>de</strong>mica nr. 4 iulie 2002 (Anul XII, 141).<br />

[27] Thierry <strong>de</strong> Montbrial, Le sens <strong>de</strong> l’histoire, Discurs <strong>de</strong> receptie la <strong>Aca<strong>de</strong>mia</strong> Română, 1999.<br />

[28] Trăuşan-Matu Ştefan, „Interfaţarea evoluată om-calculator, Bucureşti, Editura Matrix<br />

Rom, 2000.<br />

[29] Vinge Vernor, „Signs <strong>of</strong> the singularity, IEEE Spectrum, June 2008.<br />

[30] Voicu Mihai, „Secolul XXI sau Cum <strong>de</strong>scin<strong>de</strong> secolul XXI <strong>din</strong> mileniul II, Bucureşti,<br />

Editura Aca<strong>de</strong>miei Române, 2006.<br />

[31] Von Wright G.H., „Explicaţie şi înţelegere, Bucureşti, Editura Humanitas, 1995.<br />

[32] Wada Yasuo, Prospects for Single Molecule Information Processing Devices, Procee<strong>din</strong>gs<br />

<strong>of</strong> the IEEE, August 2001.<br />

[33] Wayt Gibbs W., Cybernetic Cells, Scientific American, August 2001.<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISBN 2066-8562 Vol. 5, Number 1/2012 37<br />

COMPUTATIONAL APPROACH TO DARK CURRENT<br />

SPECTROSCOPY IN CCD AS COMPLEX SYSTEMS.<br />

PART III*. DEFINITION AND USE OF A NEW PARAMETER<br />

CHARACTERIZING THE DEPLETION DARK CURRENT<br />

IN SEMICONDUCTORS<br />

I. TUNARU 1 , R. WIDENHORN 2 , E. BODEGOM 2 , D. IORDACHE 3<br />

Rezumat. Studiul efectuat a evi<strong>de</strong>nţiat faptul că frecvent rezultatele experimentale privind<br />

vitezelor <strong>de</strong> generare ale principalelor capcane adânci nu corespund valorilor prezise <strong>de</strong><br />

aproximaţia „clasică” (presupunând egalitatea secţiunilor eficace: σ n = σ p <strong>de</strong> captură a<br />

electronilor liberi şi – respectiv – golurilor) a mo<strong>de</strong>lului riguros cuantic al lui Shockley-<br />

Read-Hall (SRH). Pentru a îmbunătăţi precizia <strong>de</strong>scrierii curenţilor <strong>de</strong> întuneric <strong>de</strong> golire,<br />

lucrarea <strong>de</strong> faţă a introdus un nou parametru „gradul <strong>de</strong> polarizare a secţiunilor eficace <strong>de</strong><br />

captură a electronilor liberi, respectiv golurilor”. În afara capacităţii sale <strong>de</strong> a furniza<br />

evaluări mai exacte ale curenţilor <strong>de</strong> întuneric <strong>din</strong> semiconductori, noul parametru<br />

reprezintă un instrument util pentru: a) analiza unor „anomalii” ale valorilor vitezelor <strong>de</strong><br />

generare, b) atribuirea capcanelor cu nivele adânci pentru fiecare pixel CCD, pornind <strong>de</strong><br />

la <strong>de</strong>pen<strong>de</strong>nţa <strong>de</strong> temperatură a curenţilor <strong>de</strong> întuneric <strong>din</strong> dispozitivele CCD.<br />

Abstract. The accomplished study pointed out that frequently the experimentally observed<br />

generation rates <strong>of</strong> the main <strong>de</strong>ep-level traps do not correspond to the values predicted by<br />

the classical approximation (assuming equal capture cross-sections σ n = σ p <strong>of</strong> the free<br />

electrons and holes, respectively) <strong>of</strong> the Shockley-Read-Hall (SRH) rigorous quantum<br />

expression. In or<strong>de</strong>r to improve the accuracy <strong>of</strong> the <strong>de</strong>pletion dark current <strong>de</strong>scription, this<br />

work introduced the new parameter “polarization <strong>de</strong>gree <strong>of</strong> the capture cross-sections <strong>of</strong><br />

free electrons and holes, respectively”. Besi<strong>de</strong>s its ability to provi<strong>de</strong> consi<strong>de</strong>rably more<br />

accurate evaluations <strong>of</strong> the <strong>de</strong>pletion dark current in semiconductors, this new parameter<br />

represents a useful tool for: a) the analysis <strong>of</strong> some “anomalies” <strong>of</strong> the generation rate<br />

values, b) the assignment <strong>of</strong> <strong>de</strong>ep-level traps for each CCD pixel, starting from the<br />

experimental data concerning the temperature <strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> the dark current in CCDs.<br />

Keywords: Charge-Coupled Devices, Dark Current, Capture cross-sections <strong>of</strong> free electrons and<br />

holes, Deep-level traps<br />

1. Introduction<br />

As it is well-known, the temperature <strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> the <strong>de</strong>pletion dark current<br />

<br />

De <strong>de</strong>p (T)<br />

emitted in a semiconductor [with the intrinsic Fermi level E i the<br />

1 Ph.D. stu<strong>de</strong>nt, Physics Department, University “Politehnica” <strong>of</strong> Bucharest, Romania.<br />

2 Pr<strong>of</strong>essor, Portland State University, Oregon, USA.<br />

3 Pr<strong>of</strong>essor, Ph.D., Physics Department, University “Politehnica” <strong>of</strong> Bucharest, Romania, Honorary<br />

member <strong>of</strong> Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists.<br />

* This paper represents the continuation (3 rd part) <strong>of</strong> the works indicated by references [16].<br />

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38 Ionel Tunaru, Ralf Wi<strong>de</strong>nhorn, Erik Bo<strong>de</strong>gom, Dan Iordache<br />

generation-recombination centers (or traps) characterized by the energy level E t ,<br />

the capture cross-sections , <strong>of</strong> free electrons and holes, respectively, and<br />

n p<br />

the concentration N t ] is <strong>de</strong>scribed by the famous rigorous quantum expression <strong>of</strong><br />

Shockley, Read and Hall [1–3], by means <strong>of</strong> the generation rate U(T):<br />

x<br />

De<br />

<strong>de</strong>p<br />

<br />

<strong>de</strong>p<br />

A<br />

pix<br />

U ( T)<br />

<br />

<br />

n n<br />

ni<br />

<br />

<br />

2<br />

<br />

n<br />

pVth<br />

p n ni<br />

Nt<br />

, (1)<br />

Et<br />

Ei<br />

<br />

Ei<br />

Et<br />

<br />

exp <br />

p p ni<br />

exp <br />

kT <br />

kT <br />

where x <strong>de</strong>p is the width <strong>of</strong> the <strong>de</strong>pletion region, A pix is the area <strong>of</strong> the pixel, and n i<br />

is the intrinsic carrier concentration. Given being that besi<strong>de</strong>s the numerous<br />

physical parameters involved by expression (1), the temperature <strong>de</strong>pen<strong>de</strong>nce <strong>of</strong><br />

the <strong>de</strong>pletion dark current due to the semiconductor lattice <strong>de</strong>fects or impurities<br />

inclu<strong>de</strong>s also the parameters <strong>de</strong>scribing the temperature <strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> all<br />

physical quantities from relation (1), it results that the use <strong>of</strong> this (too intricate)<br />

expression requires to consi<strong>de</strong>r some particular cases.<br />

The most important such particular case refers to the region <strong>de</strong>pleted <strong>of</strong> carriers,<br />

where n and p n i . In this case, the expression <strong>of</strong> the <strong>de</strong>pletion dark current<br />

becomes:<br />

I<br />

<strong>de</strong>p<br />

q x<br />

<strong>de</strong>p<br />

A<br />

pix<br />

V<br />

n<br />

Et<br />

E<br />

n exp<br />

kT<br />

i<br />

p<br />

th<br />

<br />

n N<br />

i<br />

p<br />

t<br />

Ei<br />

E<br />

exp<br />

kT<br />

t<br />

. (2)<br />

From relation (2), one finds [4] that the <strong>de</strong>pletion dark current reaches a sharp<br />

maximum for the traps with energy:<br />

dI<br />

<br />

dE<br />

<strong>de</strong>p<br />

t<br />

<br />

<br />

<br />

Et,maxI <strong>de</strong>p<br />

0 <br />

E<br />

t<br />

kT n<br />

Ei<br />

ln . (3)<br />

2 <br />

Taking into account that the trap energy level E t and its capture cross-sections <strong>of</strong><br />

free electrons σ n and holes σ p , respectively, are in<strong>de</strong>pen<strong>de</strong>nt quantities, the<br />

Et Ei<br />

quantities<br />

1 n<br />

and ln are not strictly equal, but they have to be <strong>of</strong> the<br />

kT 2 <br />

p<br />

same magnitu<strong>de</strong> or<strong>de</strong>r for the <strong>de</strong>tectable traps by means <strong>of</strong> the Dark Current<br />

Spectroscopy Method (DCS) [4, 5].<br />

For this reason, the usual procedure (see e.g. [4, 6], relation (7.8), page 610) is to<br />

Et Ei<br />

take into consi<strong>de</strong>ration<br />

<br />

n<br />

and neglect ln :<br />

kT<br />

<br />

p<br />

p<br />

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Definition and Use <strong>of</strong> a New Parameter<br />

Characterizing the Depletion Dark Current in Semiconductors 39<br />

Vthni<br />

Nt<br />

U ( T)<br />

<br />

Et<br />

Ei<br />

Ei<br />

Et<br />

exp exp<br />

kT kT<br />

is not rigorous and cannot lead usually to accurate evaluations.<br />

(where: n ) (4)<br />

2. Check <strong>of</strong> the classical approximation (4) relative to the experimental results<br />

concerning the generation rate<br />

The specialty literature provi<strong>de</strong>s (e.g. the works [5]) a sufficient number <strong>of</strong><br />

experimental data about the generation rates <strong>of</strong> different <strong>de</strong>ep level traps in<br />

silicon, pointing out even the existence <strong>of</strong> some still unexplained irregularities:<br />

“… there is actually more Au present on the Mn scribe line … than there is Mn,<br />

although the stronger Mn trap dominates the dark current” [5c], p. 478.<br />

For this reason, we studied the predicted – by means <strong>of</strong> approximation (4) – ratios<br />

Et<br />

Ei<br />

<br />

U exp ( e / s)<br />

cosh<br />

/ , which should be [accor<strong>din</strong>g to relation (4)] almost<br />

kTave<br />

<br />

equal for all traps. The obtained results were synthesized by Table 1.<br />

p<br />

Table 1. Calculated values (in the frame <strong>of</strong> this work) <strong>of</strong> the “invariant” [accor<strong>din</strong>g to relation (4)]<br />

Et<br />

Ei<br />

<br />

U exp ( e / s)<br />

cosh<br />

/ , proportional to the ratio Uexp U<br />

theor<br />

kTave<br />

<br />

Trap<br />

Generation rate<br />

U exp (e/s at 55 o C)<br />

Trap level<br />

|E t – E i |<br />

(meV) [5c]<br />

Average<br />

cross-section<br />

σ (cm 2 ) [5c]<br />

U<br />

exp<br />

( e<br />

<br />

Et<br />

E<br />

/ s)<br />

cosh<br />

kTave<br />

i<br />

<br />

/<br />

<br />

Mn 6400 ~ < 50 ~ 110 -15 31074.0<br />

Ni; Co 3700 < 30 6.610 -15 1161.5<br />

Pt 970 60 710 -15 1051.0<br />

Au s 565 < 30 110 -15 1170.6<br />

Fe i 195 120150 310 -14 1461.5<br />

Trap 1<br />

(acceptor<br />

E-center)<br />

70 100 210 -15 1615.2<br />

Trap 2 8 200 810 -15 4258.3<br />

Trap 3<br />

(donor<br />

E-center)<br />

1.8 270 210 -14 9100.6<br />

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40 Ionel Tunaru, Ralf Wi<strong>de</strong>nhorn, Erik Bo<strong>de</strong>gom, Dan Iordache<br />

One finds that the approximation (4) leads to evaluations <strong>of</strong> the generation rate:<br />

(i) <strong>of</strong> the same magnitu<strong>de</strong> or<strong>de</strong>r for Ni, Co and Au (especially), as well as<br />

(though sensibly different) for the Pt, Fe i , and the acceptor E-center traps,<br />

(ii) consi<strong>de</strong>rably smaller (almost 30 times) than the experimental results<br />

for the Mn traps,<br />

(iii) sensibly smaller, but not so low as for Mn, for the traps<br />

2 (uni<strong>de</strong>ntified) and 3 (donor E-center).<br />

As it results from the more recent [7] studies <strong>of</strong> the Mn traps in Si, the most important<br />

causes <strong>of</strong> their striking strange overall behavior (see Table 1 and [5c]) are:<br />

a) the large number <strong>of</strong> Mn <strong>de</strong>fects types in Si: at least 4 different interstitial<br />

charge states Mn i , other 3 different substitutional charge states Mn s , those <strong>of</strong> the<br />

cluster Mn 4 , those <strong>of</strong> the Mn-metal (B, Al, Ga, Sn, Au) pairs (at least 2 charge<br />

states Mn-B, 2 charge states <strong>of</strong> Mn-Au, etc ; see fig. 3),<br />

b) the huge values interval <strong>of</strong> the capture cross-sections correspon<strong>din</strong>g to<br />

the different charge states <strong>of</strong> Mn <strong>de</strong>fects: starting from σ p = 210 -18 cm 2 for the<br />

E v + 0.27 eV state <strong>of</strong> Mn i , passing through the value n = 3.110 -15 cm 2 for the<br />

E c – 0.12 eV and E c – 0.43 eV states <strong>of</strong> Mn i [8], up to n = 2.110 -12 cm 2 for the<br />

level located in proximity <strong>of</strong> the Fermi level in Si [7a], the value σ ~ 10 -15 cm 2<br />

indicated by McColgin [5c] being in fact a geometric average <strong>of</strong> the Mn <strong>de</strong>fects<br />

capture cross-sections over this extremely broad interval.<br />

Accor<strong>din</strong>g to the conclusions <strong>of</strong> the [7a] work: “… Mn shows a far more complex<br />

<strong>de</strong>fect structure than Fe or Cr for instant, which do not normally exist in the<br />

substitutional form and also exhibit one single interstitial energy level in the Si band<br />

gap. A consequence <strong>of</strong> these additional energy levels for Mn is that is difficult to state<br />

a priori which level dominates recombination, as the populations <strong>of</strong> the various<br />

charge states will <strong>de</strong>pend on the Fermi level, i.e. on the doping type and<br />

concentration”. It results that the approximation (4) should be replaced by a<br />

consi<strong>de</strong>rably more accurate one, which will be <strong>of</strong> special interest for the other<br />

<strong>de</strong>ep-level traps (Ni, Co, Pt, Au s , and even for the Fe i and the acceptor E-center trap).<br />

3. Definition <strong>of</strong> the new parameter “polarization <strong>de</strong>gree <strong>of</strong> capture<br />

cross-sections”<br />

Instead <strong>of</strong> the above approximation, this work has written (without any additional<br />

approximation) the expression (2) as:<br />

I<br />

<strong>de</strong>p<br />

q x<br />

<strong>de</strong>p<br />

A<br />

pix<br />

<br />

n<br />

<br />

p<br />

V<br />

2<br />

th<br />

n N<br />

i<br />

t<br />

Et<br />

E<br />

sec h<br />

kT<br />

i<br />

<br />

pdg<br />

, (5)<br />

<br />

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Definition and Use <strong>of</strong> a New Parameter<br />

Characterizing the Depletion Dark Current in Semiconductors 41<br />

where sec h ( x)<br />

is the hyperbolic secant function:<br />

1<br />

sec h(<br />

x)<br />

. (6)<br />

cosh x<br />

The new parameter “polarization <strong>de</strong>gree <strong>of</strong> the capture cross-sections <strong>of</strong> free<br />

electrons and holes, respectively” (pdg), <strong>de</strong>scribing the asymmetry <strong>of</strong> the pair <strong>of</strong><br />

capture cross-sections , was <strong>de</strong>fined by this work as:<br />

n p<br />

p <br />

pdg <br />

arg tanh<br />

<br />

n<br />

<br />

n<br />

p<br />

p<br />

1 n<br />

ln<br />

2 <br />

p<br />

1<br />

. (7)<br />

Figure 1 below presents the plots <strong>of</strong> the function sec h(<br />

x p)<br />

for different values<br />

<strong>of</strong> the variable x and <strong>of</strong> the parameter p <strong>of</strong> the magnitu<strong>de</strong> or<strong>de</strong>r <strong>of</strong> 1. Taking into<br />

account the consi<strong>de</strong>rable <strong>de</strong>viations from the values <strong>of</strong> the previous factor<br />

Et<br />

Ei<br />

<br />

Et<br />

Ei<br />

<br />

sec h<br />

<strong>of</strong> the function sec h<br />

kT<br />

pdg , even for the very-<strong>de</strong>ep<br />

<br />

kT <br />

level traps <strong>de</strong>tectable by the DCS method, significant corrections <strong>of</strong> the <strong>de</strong>pletion<br />

dark current evaluations are expected to be brought by the expression (5).<br />

Fig. 1. Plots <strong>of</strong> the hyperbolic secant function sech(x + p) for different values <strong>of</strong> the parameters<br />

x ( Et Ei<br />

) ( kT)<br />

and p pdg (polarization <strong>de</strong>gree <strong>of</strong> the capture cross-sections).<br />

The thick vertical line through x = +2 indicates the <strong>de</strong>scent <strong>of</strong> the sech(x + p) function<br />

from the value +1 for p = 2, up to less than + 0.05 for p = + 2.5.<br />

1 The traps <strong>of</strong> the crystalline lattice (embed<strong>de</strong>d nano-particles/systems, nano-<strong>de</strong>fects) capture both<br />

free electrons and holes, but with different probabilities. Given being the capture probability is<br />

proportional to the correspon<strong>din</strong>g cross-section (σ n or σ p ), the capture probability asymmetry can<br />

be given by the expression (7) [somewhat similar to those from Optics, Nuclear physics, etc.],<br />

because: pdg > 0 corresponds to prevalent free electrons capture, pdg = 0 to equal capture<br />

probabilities, etc.<br />

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42 Ionel Tunaru, Ralf Wi<strong>de</strong>nhorn, Erik Bo<strong>de</strong>gom, Dan Iordache<br />

4. Existing experimental results about both capture cross-sections (<strong>of</strong> free<br />

electrons and holes, respectively) and their polarization <strong>de</strong>gree (pdg)<br />

Despite: a) the high technical interest presented by the i<strong>de</strong>ntification <strong>of</strong><br />

contaminants (see e.g. [5], [6]), b) the possibility to <strong>de</strong>termine experimentally<br />

both capture rates for a given trap (by means <strong>of</strong> the DLTS method [9], especially),<br />

in practice there were evaluated: (i) usually up only the (geometrical) averages<br />

n p<br />

, (ii) both capture cross-sections only for a part <strong>of</strong> the different studied<br />

traps. Table 2 synthesizes some known values <strong>of</strong> both capture cross-sections <strong>of</strong><br />

free electrons and holes, respectively, by certain <strong>de</strong>fects (traps) from silicon, as<br />

well as <strong>of</strong> their polarization <strong>de</strong>gree (pdg), implicitly. In or<strong>de</strong>r to un<strong>de</strong>rstand easier<br />

the location <strong>of</strong> the different <strong>de</strong>fects (traps) in Si, instead to indicate their positions<br />

relative to the upper limit <strong>of</strong> the valence band (Ev) or to the bottom limit <strong>of</strong> the<br />

conduction band (E c ), we give in Table 2 the evaluated traps energies relative to<br />

the intrinsic Fermi level, consi<strong>de</strong>red as E i ≈ 0.54 eV [4].<br />

Table 2. Some known values <strong>of</strong> both capture cross-sections <strong>of</strong> free electrons and holes,<br />

respectively, in silicon, as well as <strong>of</strong> their polarization <strong>de</strong>gree (pdg), implicitly<br />

Trap<br />

Group<br />

Energy<br />

(eV)<br />

σ n<br />

(cm 2 )<br />

σ p<br />

(cm 2 )<br />

k<br />

= n / p<br />

pdg<br />

Ref.<br />

U (55C)<br />

e/s [5c]<br />

+<br />

Ti i<br />

++<br />

Ti i<br />

++<br />

V i<br />

++<br />

Cr i<br />

4 E i + 0.27 3.110 -14 1.410 -15 22.14 +1.549 [7d]<br />

4 E i 0.28 1.310 -14 2.810 -17 464.3 +3.070 [7d]<br />

5 E i 0.18 5.010 -14 3.010 -18 16667 +4.86 [7d]<br />

6<br />

E i + 0.32 2.310 -13 1.110 -13 2.091 +0.369 [7d]<br />

E i + 0.30 2.010 -14 4.010 -15 5 +0.805 [10a]<br />

(Cr i + B s<br />

-<br />

) - 6; 13 E i 0.26 5.010 -15 1.010 -14 0.5 0.3466 [10a]<br />

+<br />

Mo i<br />

+<br />

Mn i<br />

E i 0.26 1.610 -14 6.010 -16 26.67 +1.642 [10b]<br />

6<br />

E i 0.223 7.810 -15 6.010 -16 13 +1.282 [8b]<br />

7 E i + 0.09 9.4 +1.1204 [7a]<br />

(Mn i + B s - ) + 7; 13 E i + 0.01 2.110 -12 3.510 -13 6.0 +1.282 [7a]<br />

Mn i<br />

++<br />

7 E i 0.21<br />

23.1<br />

(18.528.3)<br />

+1.57 [7a]<br />

all Mn<br />

Traps 7 = ( min· max ) 1/2 ≈ 1.010 -15 ; max / min ~ 10 6 [5c],<br />

[7a]<br />

Fe i<br />

+<br />

8 E i 0.16 5.010 -14 7.010 -17 714.3 +3.286 [7d]<br />

6400<br />

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Definition and Use <strong>of</strong> a New Parameter<br />

Characterizing the Depletion Dark Current in Semiconductors 43<br />

(Fe I + B s<br />

-<br />

) + 8; 13<br />

Co i<br />

+<br />

Ni i<br />

+<br />

Pt s<br />

-<br />

Pt i<br />

-<br />

Pt s<br />

+<br />

Au s<br />

-<br />

Zn s<br />

- -<br />

Zn s<br />

-<br />

PVp - <br />

E-center<br />

9<br />

10<br />

E i + 0.28<br />

( 0.02)<br />

1.410 -14<br />

( 0.02)<br />

1.110 -15<br />

(0.52.5)<br />

13 +1.282 [7c]<br />

E i 0.02 = ( n· p ) 1/2 ≈ 6.610 -15 [5c] 3700<br />

10 E i + 0.31 3.410 -15 [11]<br />

10 E i + 0.02 4.510 -15 1.0910 -14 2.42 +0.442 [11] 970<br />

10 E i 0.18 5.410 -14 [11]<br />

11<br />

E i 0.01 1.410 -16 7.610 -15 0.01842 - 1.997 [7d]<br />

5.010 -16 1.010 -15<br />

T - 4 0.5 -0.3466 [12c] 565<br />

12 E i + 0.07 1.310 -19 6.610 -15 1.9710 - 5 -5.417 [7d]<br />

12 E i 0.21 1.510 -15 4.410 -15 0.3409 - 0.538 [7d]<br />

14<br />

E i + 0.10 = ( n· p ) 1/2 ≈ 6.610 -15 [13a] 70<br />

E i + 0.084 3.710 -16 [13b]<br />

PV + 14 E i 0.27 [13a] 1.8<br />

From Table 2 (see e.g. the results referring to the traps Cr i ++ , Mo i + , Au s - , PV-pair - <br />

acceptor E-center), there result also the accuracies (not too good) <strong>of</strong> the capture crosssections<br />

evaluations, and <strong>of</strong> their polarization <strong>de</strong>gree. One finds also that the<br />

recombination rate U was not still measured systematically. Given being the capture<br />

cross-sections and their polarization <strong>de</strong>gree pdg are <strong>of</strong>ten temperature <strong>de</strong>pen<strong>de</strong>nt,<br />

table 3 synthesizes the main types <strong>of</strong> the temperature <strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> the capture<br />

cross-sections.<br />

Table 3. Main types <strong>of</strong> the temperature <strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> the capture cross sections <strong>of</strong> free electrons<br />

and/or holes, respectively in different semiconductors<br />

The type <strong>of</strong> the<br />

temperature <strong>de</strong>pen<strong>de</strong>nce<br />

Typical expression <strong>of</strong><br />

temperature <strong>de</strong>pen<strong>de</strong>nce<br />

Some examples for the<br />

traps in the semiconductor<br />

Reference<br />

Arrhenius law n (T) n exp(-E B /kT) EL2, HL1, HL10 in GaAs [14a]<br />

Power laws (T) T -n n 2.5 ( n, Au in p-Si) [12c]<br />

n 0.21 ( n, Au in n-Si) [12d]<br />

Temperature<br />

in<strong>de</strong>pen<strong>de</strong>nce<br />

(T) constant<br />

n 4.0 ( p, Au in n-Si)<br />

p in GaAs<br />

n, Au in n-Si<br />

[12c]<br />

[14a]<br />

[12c]<br />

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44 Ionel Tunaru, Ralf Wi<strong>de</strong>nhorn, Erik Bo<strong>de</strong>gom, Dan Iordache<br />

5. Experimental evaluation <strong>of</strong> the difference E t – E i<br />

In or<strong>de</strong>r to interpret the obtained (calculated) values <strong>of</strong> E t – E i correspon<strong>din</strong>g<br />

sometimes to a mixture <strong>of</strong> <strong>de</strong>fects insi<strong>de</strong> each studied pixel, an experimental<br />

evaluation <strong>of</strong> the difference E t – E i is necessary. Given being that the most<br />

efficient experimental method inten<strong>de</strong>d to the <strong>de</strong>fects location insi<strong>de</strong> the studied<br />

semiconductor forbid<strong>de</strong>n band is the <strong>de</strong>ep-level transient spectroscopy (DLTS)<br />

method, we have to evaluate the E t – E i difference starting from the <strong>de</strong>fects (traps)<br />

positions relative to the upper limit E v <strong>of</strong> the valence band and the bottom limit<br />

(edge) E c <strong>of</strong> the conduction one (see fig. 2).<br />

Fig. 2. Positions <strong>of</strong> the <strong>de</strong>fects (traps) energy levels and <strong>of</strong> the Fermi intrinsic level<br />

accor<strong>din</strong>g to the DLTS results.<br />

Given being for a certain temperature T the energy gap is (approximately) known,<br />

it is necessary to evaluate also the intrinsic Fermi energy E i (T) at this temperature.<br />

Accor<strong>din</strong>g to the basic Con<strong>de</strong>nsed Matter Physics treatises [2], the temperature<br />

<strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> the intrinsic Fermi energy E i (T) is given by the expression:<br />

where:<br />

*<br />

dp<br />

*<br />

dn<br />

1 3kT<br />

m<br />

Ei<br />

( T)<br />

Eg<br />

( T)<br />

ln , (8)<br />

2 4 m<br />

2/3<br />

* * 3/ 2 * 3/ 2<br />

m<br />

<br />

<br />

dp m pl m ph and:<br />

<br />

<br />

m<br />

*<br />

dn<br />

3 * 2 *<br />

6mt<br />

ml<br />

(9)<br />

are the effective masses correspon<strong>din</strong>g to the states <strong>de</strong>nsities <strong>of</strong> holes and free<br />

* * * *<br />

electrons, respectively, while m pl, mph,<br />

ml<br />

and m t are the effective masses<br />

associated to the light and heavy holes, respectively, and to the longitu<strong>din</strong>al and<br />

transverse electrons effective masses, relative to the major axis <strong>of</strong> the energy<br />

ellipsoid E( k ). For free electrons in silicon, there are used the values<br />

ml * 0. 98 m o , mt<br />

* 0. 19 m o , and ml<br />

* 0. 916 m o , mt<br />

* 0. 225 m o , which lead to<br />

the values mdn<br />

* 1 0. 5965 mo<br />

and *<br />

mdn<br />

2 0. 6528 m o <strong>of</strong> the effective mass<br />

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Definition and Use <strong>of</strong> a New Parameter<br />

Characterizing the Depletion Dark Current in Semiconductors 45<br />

associated to the electrons state <strong>de</strong>nsity in the conduction band <strong>of</strong> Si, while for the<br />

holes from Si there are usually used the values m * pl 0. 16 mo<br />

, *<br />

mph<br />

0. 49 m o ,<br />

which lead to the value<br />

m * 0. 5492 m <strong>of</strong> the effective mass associated to the<br />

dp<br />

holes state <strong>de</strong>nsity in the silicon valence band. As we use the first or the second<br />

o<br />

3 mdp<br />

pair <strong>of</strong> electron effective mass in Si, we obtain ln 0.<br />

06196 , or – 0.1296,<br />

4<br />

*<br />

mdn<br />

hence the temperature coefficient <strong>of</strong> the silicon intrinsic Fermi energy correction:<br />

3<br />

*<br />

k mdp<br />

5<br />

1<br />

4<br />

ln<br />

dn<br />

1.11610<br />

K<br />

*<br />

is at least one magnitu<strong>de</strong> or<strong>de</strong>r less than that <strong>of</strong> the<br />

energy gap correspon<strong>din</strong>g to silicon: E g , Si ( T)<br />

1.21<br />

4.2 10<br />

T ( eV ) [2].<br />

For an average use temperature T ≈ 250 K (this work, [12a], etc.), one finds that<br />

3kT<br />

m<br />

the intrinsic Fermi energy correction ln has a value insi<strong>de</strong> the interval<br />

4 m<br />

(1.34; 2.8) meV, remaining so negligible relative to the usual <strong>de</strong>fects (traps)<br />

energies in Si, even for the very-<strong>de</strong>ep level <strong>de</strong>fects, <strong>de</strong>tectable by the studied dark<br />

current spectroscopy method.<br />

6. On the evaluation <strong>of</strong> the polarization <strong>de</strong>gree <strong>of</strong> capture cross-sections <strong>of</strong><br />

free electrons and holes, respectively<br />

Taking into account that the power law expressions <strong>of</strong> the temperature<br />

<strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> capture cross-sections can be approximated by Arrhenius type<br />

expressions (with negative activation energy E B ) and substituting the Arrhenius<br />

expression [see Table 3] in the polarization <strong>de</strong>gree <strong>de</strong>finition (7), one obtains:<br />

1 n ( T)<br />

1 n<br />

EB<br />

EB<br />

pdg( T)<br />

ln ln pdg<br />

, hence the temperature<br />

2 ( T)<br />

2 2kT<br />

2kT<br />

p<br />

p<br />

<strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> the hyperbolic secant argument can be expressed as:<br />

E <br />

<br />

E E<br />

t Ei<br />

Et<br />

Ei<br />

EB<br />

/ 2<br />

t i eff<br />

arg sec h(<br />

T)<br />

pdg(<br />

T)<br />

<br />

pdg<br />

<br />

pdg<br />

, (10)<br />

kT<br />

kT<br />

kT<br />

by means <strong>of</strong> the effective energies difference Et E i eff<br />

and <strong>of</strong> the pdg(T)<br />

asymptotic value<br />

pdg .<br />

The DCS method allows however an indirect evaluation <strong>of</strong> the “polarization<br />

<strong>de</strong>gree” pdg (in fact <strong>of</strong> its asymptotic value pdg ), starting from the improved<br />

*<br />

dp<br />

*<br />

dn<br />

<br />

<br />

4<br />

<br />

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46 Ionel Tunaru, Ralf Wi<strong>de</strong>nhorn, Erik Bo<strong>de</strong>gom, Dan Iordache<br />

approximation (5). Our (indirect) evaluation <strong>of</strong> the effective parameters |E t – E i | eff<br />

and pdg ∞ was achieved by means <strong>of</strong> the least-squares fit (using the gradient<br />

method) <strong>of</strong> the slope s and intercept i <strong>of</strong> the regression line <strong>of</strong> the modulus <strong>of</strong> the<br />

argument <strong>of</strong> the hyperbolic secant function in terms <strong>of</strong> the kT<br />

1 parameter:<br />

Et<br />

Ei<br />

<br />

1<br />

arg sec<br />

h<br />

pdg s i<br />

kT<br />

. (11)<br />

<br />

<br />

kT<br />

In or<strong>de</strong>r to provi<strong>de</strong> correct interpretations <strong>of</strong> the results <strong>of</strong> our procedure (10), we<br />

studied the existing experimental data for 20 randomly chosen pixels <strong>of</strong> a Spectra<br />

Vi<strong>de</strong>o CCD camera (mo<strong>de</strong>l SV512V1) manufactured by Pixelvision, Inc. (see<br />

[9a]). The obtained (in the frame <strong>of</strong> this work) types <strong>of</strong> qualitative results and<br />

their interpretations are synthesized by Table 4.<br />

Table 4. Main types <strong>of</strong> results obtained by means <strong>of</strong> the regression line<br />

|arg[sech(pdg+(E t -E i )/kT]|= i + s/kT study and their interpretation<br />

Slope s<br />

sign<br />

Intercept i<br />

sign<br />

> 0 > 0<br />

> 0 < 0<br />

< 0 > 0<br />

Interpretation<br />

Both (E t – E i ) eff and pdg ∞ have the same sign, hence:<br />

|E t – E i | eff = s, |pdg| ∞ = i and: (E t – E i ) eff /pdg ∞ > 0<br />

(E t – E i ) eff /kT > - pdg ∞ > 0 or<br />

(E t – E i ) eff /kT < - pdg ∞ < 0<br />

pdg ∞ > - (E t – E i ) eff /kT = (E i – E t ) eff /kT > 0 or<br />

pdg ∞ < - (E t – E i ) eff /kT = (E i – E t ) eff /kT < 0<br />

Examples <strong>of</strong><br />

pixels [12a]<br />

188; 471<br />

121; 200<br />

321; 400<br />

In or<strong>de</strong>r to estimate the “impact” <strong>of</strong> the polarization <strong>de</strong>gree (pdg) values on the<br />

<strong>de</strong>pletion dark current the obtained numerical results for the 17 pixels whose data<br />

sets lead to physically convergent evaluations were synthesized by Table 5. As<br />

one can find easily, the accuracy <strong>of</strong> the obtained results <strong>de</strong>creases very much for<br />

the pixels emitting weak <strong>de</strong>pletion dark current (low values <strong>of</strong> the <strong>de</strong>pletion preexponential<br />

factor, Dep).<br />

Table 5. Interpretation <strong>of</strong> the obtained quantitative (numerical) results [s = sign(E t -E i ) eff ]<br />

Pixel<br />

Obtained information about<br />

Dep (Mcps·K -3/2 ), the effective parameters<br />

10 6 counts/s·K -3/2 |E t – E i | eff , meV s·pdg ∞<br />

Calc. Depletion<br />

Dark Current<br />

Accuracy (%)<br />

sech[pdg+<br />

(E t -E i )/kT]<br />

321; 400 2.541 32.125 3.075 17.47% 0.3808<br />

181; 260 5.433 24.39 0.0187 2.975% 0.5887<br />

121; 200 6.022 34.44 0.3274 5.65% 0.5381<br />

141; 220 6.478 8.49 0.773 6.158% 0.5872<br />

101; 180 6.623 24.66 0.0455 2.454% 0.5702<br />

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Definition and Use <strong>of</strong> a New Parameter<br />

Characterizing the Depletion Dark Current in Semiconductors 47<br />

301; 380 7.224 30.85 0.3114 3.002% 0.6068<br />

188; 471 9.530 28.04 0.790 6.988% 0.2511<br />

81; 160 11.710 33.59 0.0154 2.294% 0.4117<br />

221; 300 15.998 28.03 0.438 3.797% 0.2176<br />

201; 280 21.944 31.21 0.117 1.77% 0.4140<br />

29; 88 32.120 51.860 0.155 2.473% 0.2207<br />

61; 140 40.792 27.352 1.369 7.055% 0.1467<br />

281; 360 66.386 45.697 0.397 3.197% 0.1688<br />

261; 340 105.688 57.225 0.135 2.2798% 0.1306<br />

341; 420 254.039 55.479 0.259 2.277% 0.1249<br />

161; 240 268.671 76.223 0.632 3.73% 0.0338<br />

31; 247 421.361 2.16 1.3896 5.379% 0.5109<br />

Figures 3 and 4 present the diagrams <strong>of</strong> the traps levels for GaAs and Mn in the Si<br />

lattice, respectively. From Table 2, one finds that the majority <strong>of</strong> donor /acceptor<br />

states are located in the upper/lower half <strong>of</strong> the forbid<strong>de</strong>n band, respectively,<br />

while the other states – named here “trans-Fermi level donor/ acceptor states” (as<br />

the levels EL2, E5, HL10, HL16 in GaAs, (Mn + Au - ) + and Mn ++ i in the Si lattice)<br />

have negative values <strong>of</strong> the product pdg sign( E E ) .<br />

t<br />

i<br />

Fig. 3. Traps levels diagram for GaAs [14a].<br />

Fig. 4. Traps levels diagram for Mn in the silicon lattice [7, 8, 15].<br />

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48 Ionel Tunaru, Ralf Wi<strong>de</strong>nhorn, Erik Bo<strong>de</strong>gom, Dan Iordache<br />

Taking into account that the number <strong>of</strong> the “trans-Fermi level states” is sensibly<br />

less than the number <strong>of</strong> the other electronic states, this fin<strong>din</strong>g represents a useful<br />

tool in the assignment <strong>of</strong> these states (traps).<br />

6. Study <strong>of</strong> the “anomalies” <strong>of</strong> the generation rate U values<br />

This work achieved the least-squares fit (using the gradient method [17], [16b]) <strong>of</strong><br />

the improved approximation (5):<br />

De<br />

<br />

De<br />

<br />

0 , diff<br />

T<br />

3<br />

Eg<br />

<br />

exp <br />

<br />

De<br />

kT <br />

<br />

0, <strong>de</strong>p<br />

T<br />

3/ 2<br />

Eg<br />

(<br />

Et<br />

Ei<br />

)<br />

exp <br />

<br />

sec h<br />

2kT<br />

kT<br />

eff<br />

pdg<br />

<strong>of</strong> the experimental results concerning the dark current emitted by some pixels <strong>of</strong><br />

the studied Spectra Vi<strong>de</strong>o CCD camera (mo<strong>de</strong>l SV512V1) [12a].<br />

There were obtained evaluations <strong>of</strong> all parameters <strong>of</strong> the above expression, particularly<br />

<strong>of</strong> the <strong>de</strong>pletion pre-exponential factor<br />

<br />

De 0 , <strong>de</strong>p Dep , effective energy gap E g and <strong>of</strong><br />

the trap location ( E ) insi<strong>de</strong> the silicon forbid<strong>de</strong>n band, as well as <strong>of</strong> the<br />

t E i<br />

eff<br />

asymptotic value pdg <strong>of</strong> the capture cross-sections polarization <strong>de</strong>gree. Using these<br />

numerical estimations, the numerical evaluation <strong>of</strong> the generation rate at the<br />

temperature t 55 C (hence T gr = 328.15 K) was obtained by means <strong>of</strong> the expression:<br />

gr<br />

U(<br />

T<br />

gr<br />

<br />

<br />

<br />

3/ 2<br />

E<br />

<br />

g ( E<br />

<br />

t Ei<br />

) eff<br />

) De0 , <strong>de</strong>pTgr<br />

exp sec<br />

h<br />

pdg<br />

. (12)<br />

<br />

2kTgr<br />

<br />

kTgr<br />

<br />

The obtained results are presented in Table 6, where the pixels were written in the<br />

monotonic or<strong>de</strong>r <strong>of</strong> their increasing <strong>de</strong>pletion pre-exponential factors Dep. While –<br />

accor<strong>din</strong>g to the classical approximation (4) – it was expected to find the<br />

proportionality <strong>of</strong> the generation rate U(T) with the <strong>de</strong>pletion pre-exponential factor<br />

<br />

<strong>de</strong>p<br />

Dep De0 , , the examination <strong>of</strong> Table 6 points out several discontinuities, that<br />

can be explained only by the different values <strong>of</strong> polarization <strong>de</strong>gree pdg and <strong>of</strong> the<br />

effective energies difference Et E i eff<br />

.<br />

Table 6. Comparison <strong>of</strong> the evaluated values <strong>of</strong> the <strong>de</strong>pletion pre-exponential factor Dep and <strong>of</strong> the<br />

generation rate (correspon<strong>din</strong>g hyperbolic secant function values in brackets) for different<br />

pixels <strong>of</strong> a SpectraVi<strong>de</strong>o CCD camera (mo<strong>de</strong>l SV512V1)<br />

Pixel<br />

Dep (Mcps K 3/2 Evaluated<br />

),<br />

10 6 counts/s·K 3/2 generation rate<br />

U(e - /s) at 55C<br />

Pixel<br />

<br />

<br />

<br />

<br />

Dep (Mcps K -3/2 Evaluated<br />

),<br />

10 6 counts/s·K 3/2 generation rate<br />

U(e - /s) at 55C<br />

321; 400 2.541 124.6 (0.3808) 201; 280 21.944 2243 (0.4140)<br />

181; 260 5.433 680 (0.5887) 29; 88 32.120 1981 (0.2207)<br />

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Definition and Use <strong>of</strong> a New Parameter<br />

Characterizing the Depletion Dark Current in Semiconductors 49<br />

121; 200 6.022 866 (0.5381) 61; 140 40.792 1464 (0.1467)<br />

141; 220 6.478 713.5 (0.5872) 281; 360 66.386 3184 (0.1688)<br />

101; 180 6.623 751 (0.5702) 261; 340 105.688 3276 (0.1306)<br />

301; 380 7.224 1564 (0.6068) 341; 420 254.039 3899 (0.1249)<br />

188; 471 9.530 588 (0.2511) 161; 240 268.671 1996 (0.0338)<br />

81; 160 11.710 1176 (0.4117) 31; 247 421.361 4923 (0.5109)<br />

221; 300 15.998 1654 (0.2176)<br />

The consi<strong>de</strong>rable impact <strong>of</strong> the polarization <strong>de</strong>gree (pdg) on the values <strong>of</strong> the<br />

Et<br />

Ei<br />

eff<br />

<br />

hyperbolic secant sec h<br />

pdg and <strong>of</strong> the generation rate, is<br />

<br />

kT<br />

<br />

indicated both by the values <strong>of</strong> the last column <strong>of</strong> Table 5 (see the value for the<br />

pixel 161; 240, particularly) and <strong>of</strong> Fig. 1.<br />

Accor<strong>din</strong>g to the work [5c], the even more striking large generation rates <strong>of</strong> the Mn,<br />

Ni, Co traps (see e.g. Table 1) could be explained by means <strong>of</strong> a complex character<br />

(like Mn 4 ) <strong>of</strong> these traps and/or <strong>of</strong> a possible Poole-Frenkel [18] effect. The<br />

accomplished analysis pointed out that even the capture cross-sections <strong>of</strong> the Ni and<br />

Co traps are consi<strong>de</strong>rably larger than that <strong>of</strong> the substitutional gold Au s , their<br />

generation rates agree very well [accor<strong>din</strong>g to the classical approximation (4), see<br />

Table 1, with that <strong>of</strong> Au s , while even the use <strong>of</strong> the improved approximation (5) does<br />

not lead to a quantitative justification <strong>of</strong> the experimental value <strong>of</strong> the Mn trap<br />

generation rate.<br />

Given being the: a) consi<strong>de</strong>rably more complex <strong>de</strong>fect structure (larger number <strong>of</strong><br />

charge states) <strong>of</strong> Mn than those <strong>of</strong> Cr, Fe, Ni, Co, etc, b) still incompletely<br />

characterized (mainly by means <strong>of</strong> the capture cross sections <strong>of</strong> free electrons and<br />

holes, respectively) <strong>of</strong> many Mn <strong>de</strong>fects (e.g. <strong>of</strong> the substitutional states, <strong>of</strong> the<br />

Mn 4 cluster, <strong>of</strong> the Mn pairs with Al, Ga, Sn, etc), c) intentional contamination<br />

with Mn atoms which lead to the McColgin’s results [5c], our analysis lead to the<br />

conclusion that the striking strange pair <strong>of</strong> values referring to the average crosssection<br />

σ and to the generation rate/Mn atom can be explained (more than by the<br />

Poole-Frenkel effect) by an averaging <strong>of</strong> the generation rates <strong>of</strong> Mn <strong>de</strong>fects in<br />

different charge states with very different capture cross sections (many <strong>of</strong> them<br />

consi<strong>de</strong>rably higher than the average value indicated by [5c]).<br />

The obtainment <strong>of</strong> new experimental information about both free electrons n and<br />

holes p capture cross-sections <strong>of</strong> the main <strong>de</strong>ep-level traps in silicon will<br />

contribute <strong>of</strong> course to a more accurate <strong>de</strong>scription <strong>of</strong> the temperature <strong>de</strong>pen<strong>de</strong>nce<br />

<strong>of</strong> the <strong>de</strong>pletion dark current in semiconductors.<br />

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50 Ionel Tunaru, Ralf Wi<strong>de</strong>nhorn, Erik Bo<strong>de</strong>gom, Dan Iordache<br />

7. Use <strong>of</strong> the polarization <strong>de</strong>gree pdg as an assignment criterion <strong>of</strong> the<br />

<strong>de</strong>ep-level traps<br />

The accomplished study pointed out that the newly <strong>de</strong>fined physical parameter<br />

“polarization <strong>de</strong>gree <strong>of</strong> the capture cross-sections <strong>of</strong> free electrons and holes,<br />

respectively” is a basic feature <strong>of</strong> the <strong>de</strong>ep-level traps, allowing consi<strong>de</strong>rably more<br />

accurate <strong>de</strong>scriptions <strong>of</strong> the temperature <strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> the <strong>de</strong>pletion dark current<br />

in charge-coupled <strong>de</strong>vices.<br />

For this reason, we consi<strong>de</strong>r that besi<strong>de</strong>s the classical assignment criteria as the:<br />

<br />

a) <strong>de</strong>pletion pre-exponential factor De 0 , <strong>de</strong>p , b) generation rate U(T g.r. ) at a given<br />

temperature, c) the location <strong>of</strong> the studied trap insi<strong>de</strong> the semiconductor forbid<strong>de</strong>n<br />

band, d) average capture cross-section , the: e) polarization<br />

<strong>de</strong>gree<br />

1<br />

pdg ln<br />

2<br />

<br />

<br />

n<br />

p<br />

n p<br />

arg tanh<br />

<br />

f) average value h(<br />

E E ) kT pdg <br />

n<br />

t i eff /<br />

p<br />

ave<br />

ave<br />

n<br />

p<br />

<strong>of</strong> capture cross-sections, as well as the:<br />

sec <strong>of</strong> the hyperbolic secant function,<br />

are also basic assignment criteria for the <strong>de</strong>ep-level traps in a semiconductor,<br />

starting from the observed temperature <strong>de</strong>pen<strong>de</strong>nce <strong>of</strong> the dark current in each<br />

CCD pixel (the Dark Current Spectroscopy method).<br />

Conclusions<br />

This work pointed out the necessity to introduce the new parameter “polarization<br />

<strong>de</strong>gree <strong>of</strong> the capture cross-sections <strong>of</strong> free electrons and holes, respectively” in<br />

or<strong>de</strong>r to ensure a sufficiently accurate <strong>de</strong>scription <strong>of</strong> the temperature <strong>de</strong>pen<strong>de</strong>nce<br />

<strong>of</strong> the <strong>de</strong>pletion dark current in semiconductors. It was found also the ability <strong>of</strong><br />

this new parameter to: a) analyze successfully the “anomalies” <strong>of</strong> some reported<br />

generation rate values [e.g., no anomaly for the reported generation rates <strong>of</strong> Ni and<br />

Co [5c], but probably wrong value (1210 14 cm 2 , instead <strong>of</strong> ~ 110 15 cm 2 ) for<br />

the average cross-section <strong>of</strong> the electronic states <strong>of</strong> the embed<strong>de</strong>d Mn traps which<br />

produce a 6400 e - /s generation rate], b) discriminate among the contributions <strong>of</strong><br />

the different <strong>de</strong>ep-level traps to the <strong>de</strong>pletion dark current in each CCD pixel,<br />

allowing so certain assignments <strong>of</strong> the <strong>de</strong>ep-level traps in the CCDs pixels. In this<br />

aim, both newly introduced notions <strong>of</strong> “polarization <strong>de</strong>gree” and “trans-Fermi<br />

level donor/acceptor states” are useful.<br />

Acknowledgements<br />

The authors thank very much for the fruitful discussions and important received<br />

information to Dr. G. Moagar-Paladian, National Institute for Research and<br />

Development in Micro-technology, Bucharest.<br />

<br />

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Definition and Use <strong>of</strong> a New Parameter<br />

Characterizing the Depletion Dark Current in Semiconductors 51<br />

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[16] a) R. Wi<strong>de</strong>nhorn, E. Bo<strong>de</strong>gom, D. Iordache, I. Tunaru, Computational Approach to Dark<br />

Current Spectroscopy in CCDs as Complex Systems. I. Experimental Part and Choice <strong>of</strong> the<br />

Uniqueness Parameters", in the Scientific Bulletin <strong>of</strong> "Politehnica" University Bucharest, Series A:<br />

Applied Mathematics and Physics, vol. 72, no. 4, 2010, pp. 197-208; b) I. Tunaru, R. Wi<strong>de</strong>nhorn,<br />

D. Iordache, E. Bo<strong>de</strong>gom, ibid. II. Numerical Analysis <strong>of</strong> the Uniqueness Parameters Evaluation,<br />

ibid., 73(1) 149-162(2011).<br />

[17] a) K. Levenberg, A method for the solution <strong>of</strong> certain problems in least squares, Quarterly <strong>of</strong><br />

Applied Mathematics, vol. 2, 1944, pp. 164–168; b) D. W. Marquardt, An algorithm for leastsquares<br />

estimation <strong>of</strong> nonlinear parameters, Journal <strong>of</strong> the Society for Industrial and Applied<br />

Mathematics, vol. 11, no. 2, 1963, pp. 431–441; c) N. Andrei, Another Conjugate Gradient<br />

Algorithm for Unconstrained Optimization, Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, Series<br />

on Science and Technology <strong>of</strong> Information, vol. 1, no. 1, 2008, pp. 7-20.<br />

[18] A. Sevcenco, Gh. Brezeanu, An accurate analytical mo<strong>de</strong>l with a reduced parameter set for<br />

short-channel MOS transistors, Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, Series on Science<br />

and Technology <strong>of</strong> Information, vol. 2, no. 1, 2009, pp. 107-120.<br />

[19] a) J. Frenkel, On pre-breakdown phenomena in insulators and semiconductors, in Phys. Rev.<br />

vol. 54, 1938, p. 647; b) J. van <strong>de</strong>r Spiegel, G. J. Declerk, Characterization <strong>of</strong> Dark Current Non-<br />

Uniformities in CCDs, in Solid-State Electronics, vol. 27(2) 1984, pp. 147-154; c) W. E. Meyer,<br />

Digital DLTS studies on radiation induced <strong>de</strong>fects in Si, GaAs and GaN, PhD Diss., Univ. <strong>of</strong><br />

Pretoria (South-Africa), Nov. 2006; d) E. A. G. Webster, R. Nicol, L. Grant, D. Renshaw,<br />

Validated Dark Spectroscopy on a per-pixel basis in a CMOS image sensors, Proc. International<br />

Image Sensor Workshop, Bergen (Norway), 26-28 July 2009.<br />

[20] A. Danchiv, M. Bo<strong>de</strong>a, Cl. Dan, Chopper Stabilization Techniques, part I: Chopper Amplifier<br />

Topologies Overview, Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, Series on Science and<br />

Technology <strong>of</strong> Information, vol. 1, no. 1, 2008, pp. 31-42.<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066-8562 Volume 5, Number 1/2012 53<br />

AUTOMATIC COMPUTER<br />

MUSIC CLASSIFICATION AND SEGMENTATION<br />

Adrian SIMION 1 , Stefan TRAUSAN-MATU 2<br />

Rezumat. Lucrarea <strong>de</strong> faţă <strong>de</strong>scrie şi aplică diferite meto<strong>de</strong> pentru segmentarea<br />

automată a muzicii realizată cu ajutorul unui calculator. Pe baza rezultatelor şi a<br />

tehnicilor <strong>de</strong> extragere a caracteristicilor folosite, se încearcă <strong>de</strong> asemenea o<br />

clasificare/recunoaştere a fragmentelor folosite. Algoritmii au fost testaţi pe seturile <strong>de</strong><br />

date Magnatune şi MARSYAS, dar instrumentele s<strong>of</strong>tware implementate pot fi folosite pe<br />

o gamă variată <strong>de</strong> surse. Instrumentele <strong>de</strong>scrise vor fi integrate într-un „framework” /<br />

sistem s<strong>of</strong>tware numit ADAMS (Advanced Dynamic Analysis <strong>of</strong> Music S<strong>of</strong>tware -<br />

S<strong>of</strong>tware pentru Analiza Dinamică Avansată a Muzicii) cu ajutorul căruia se vor putea<br />

evalua şi îmbunătăţi diferitele sarcini <strong>de</strong> analiză şi compoziţie a muzicii. Acest sistem are<br />

la bază biblioteca <strong>de</strong> programe MARSYAS şi conţine un modul similar cu WEKA pentru<br />

sarcini <strong>de</strong> procesare a datelor şi învăţare automată.<br />

Abstract. This paper <strong>de</strong>scribes and applies various methods for automatic computer<br />

music segmentation. Based on these results and on the feature extraction techniques used,<br />

is tried also a genre classification/recognition <strong>of</strong> the excerpts used. The algorithms were<br />

tested on the Magnatune and MARSYAS datasets, but the implemented s<strong>of</strong>tware tools can<br />

also be used on a variety <strong>of</strong> sources. The tools <strong>de</strong>scribed here will be subject to a<br />

framework/s<strong>of</strong>tware system called ADAMS (Advanced Dynamic Analysis <strong>of</strong> Music<br />

S<strong>of</strong>tware) that will help evaluate and enhance the various music analysis/composition<br />

tasks. This system is based on the MARSYAS open source s<strong>of</strong>tware framework and<br />

contains a module similar to WEKA for data-mining and machine learning tasks.<br />

Keywords: automatic segmentation, audio classification, music information retrieval, music<br />

content analysis, chord <strong>de</strong>tection, vocal and instrumental regions<br />

1. Music Information Retrieval<br />

The number <strong>of</strong> digital music recor<strong>din</strong>gs has a continuous growth, promoted by the<br />

users‘ interest as well as the advances <strong>of</strong> the new technologies that support the<br />

pleasure <strong>of</strong> listening to music. There are a few reasons that explain this trend, first<br />

<strong>of</strong> all, the existential characteristic <strong>of</strong> the musical language. Music is a form <strong>of</strong> art<br />

which can be shared by people that belong to different cultures because it<br />

surpasses the bor<strong>de</strong>rs <strong>of</strong> the national language and <strong>of</strong> the cultural background. As<br />

an example the West American music has many enthusiasts in Japan, and many<br />

persons in Europe appreciate the classical Indian music. These forms <strong>of</strong><br />

1 Eng., Ph.D. stu<strong>de</strong>nt, Faculty <strong>of</strong> Automatic Control and Computers, University Politehnica <strong>of</strong><br />

Bucharest, Bucharest, Romania, (simion.adrian@gmail.com).<br />

2 Correspon<strong>din</strong>g member <strong>of</strong> AOSR. Pr<strong>of</strong>., Ph.D., Faculty <strong>of</strong> Automatic Control and Computers,<br />

University Politehnica <strong>of</strong> Bucharest, Bucharest, Romania, (stefan.trausan@cs.pub.ro).<br />

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54 Adrian Simion, Ștefan Trăușan-Matu<br />

expression can be appreciated without the need <strong>of</strong> a translation that is in most <strong>of</strong><br />

the cases necessary for accessing foreign textual papers.<br />

Another reason is the fact that technology for recor<strong>din</strong>g music, digital<br />

transformation and playback allows the users access to information that is almost<br />

comparable to live performances, at least at audio quality level.<br />

Last, music is an art form that is cult and popular at the same time and sometimes<br />

is impossible to draw a line between the two, like jazz and traditional music.<br />

The high availability and <strong>de</strong>mand for music content induced new requirements<br />

about its management, advertisement and distribution. This required a more in<strong>de</strong>pth<br />

and direct analysis <strong>of</strong> the content than that provi<strong>de</strong>d by simple human<br />

driven meta-data cataloguing.<br />

The new techniques allowed approaches that were only encountered in theoretical<br />

musical analysis. One <strong>of</strong> these problems was stated by Frank Howes [1]: There is<br />

thus a vast corpus <strong>of</strong> music material available for comparative study. It would be<br />

fascinating to discover and work out a correlation between music and social<br />

phenomena. With the current processing power and advancements we can answer<br />

questions such as: What is the ethnic background <strong>of</strong> a particular piece <strong>of</strong> music or<br />

what cultures it spawns.<br />

In light <strong>of</strong> these possibilities and technological advances we nee<strong>de</strong>d a new<br />

discipline that would try to cover and answer the various problems. Music<br />

Information Retrieval (MIR) is an interdisciplinary science that retrieves its<br />

information from music. The origins <strong>of</strong> MIR are domains like: musicology,<br />

cognitive psychology, linguistic and computer science.<br />

An active research area is composed <strong>of</strong> new methods and tools for pattern fin<strong>din</strong>g<br />

as well as the comparison <strong>of</strong> musical content. The International Society for Music<br />

Information Retrieval [2] is coupled with the annual Music Information Retrieval<br />

Evaluation eXchange (MIREX) [3]. The evaluated tasks inclu<strong>de</strong> Automatic Genre<br />

I<strong>de</strong>ntification, Chord Detection, Segmentation, Melody Extraction, Query by<br />

Humming, to name a few. This paper will focus mostly on Automatic<br />

Segmentation and Genre I<strong>de</strong>ntification.<br />

2. Former studies and related work on Automatic Music Segmentation<br />

The topic <strong>of</strong> speech/music classification was studied by many researchers. While<br />

the applications can be very different, many studies use similar sets <strong>of</strong> acoustic<br />

features, such as short time energy, zero-crossing rate, cepstrum coefficients,<br />

spectral roll <strong>of</strong>f, spectrum centroid and ―loudness,‖ alongsi<strong>de</strong> some unique<br />

features, such as ―dynamism.‖ However, the exact combinations <strong>of</strong> features used<br />

can vary greatly, as well as the size <strong>of</strong> the feature set.<br />

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Automatic Computer Music Classification and Segmentation 55<br />

Typically some long term statistics, such as the mean or the variance, and not the<br />

features themselves, are used for the discrimination.<br />

The major differences between the different studies lie in the exact classification<br />

algorithm, even though some popular classifiers (K-nearest neighbor, Gaussian<br />

multivariate, neural network) are <strong>of</strong>ten used as a basis.<br />

For the studies, mostly, different databases are used for training and testing the<br />

algorithm. It is worth noting that in these studies, especially the early ones, these<br />

databases are fairly small. The following table <strong>de</strong>scribes some <strong>of</strong> the former<br />

studies:<br />

Table 1. Some <strong>of</strong> the former studies<br />

Author Application Features Classification method<br />

Automatic real-time FM Short-time energy, statistical parameters <strong>of</strong> Multivariate Gaussian<br />

radio monitoring the ZCR<br />

classifier<br />

13 temporal, spectral and cepstral features<br />

(e.g., 4Hz modulation energy, % <strong>of</strong> low Gaussian mixture mo<strong>de</strong>l<br />

Speech/music<br />

energy frames,<br />

(GMM), K nearest<br />

discrimination for<br />

spectral roll <strong>of</strong>f, spectral centroid, spectral neighbour (KNN), K-D<br />

automatic speech<br />

flux, ZCR, cepstrum-based feature, trees, multidimensional<br />

recognition<br />

―rhythmicness‖),<br />

Gaussian MAP estimator<br />

variance <strong>of</strong> features across 1 sec.<br />

Saun<strong>de</strong>rs,<br />

1996 [4]<br />

Scheirer and<br />

Slaney, 1997<br />

[5]<br />

Foote, 1997<br />

[6]<br />

Liu et al.,<br />

1997 [7]<br />

Zhang and<br />

Kuo, 1999 [8]<br />

Williams and<br />

Ellis, 1999<br />

[9]<br />

El-Malehet<br />

al., 2000 [10]<br />

Buggati et al.,<br />

2002 [11]<br />

Lu, Zhang,<br />

and Jiang,<br />

Retrieving audio<br />

documents by acoustic<br />

similarity<br />

Analysis <strong>of</strong> audio for<br />

scene classification <strong>of</strong><br />

TV programs<br />

Audio<br />

segmentation/retrieval<br />

for vi<strong>de</strong>o scene<br />

classification, in<strong>de</strong>xing<br />

<strong>of</strong> raw audio visual<br />

recor<strong>din</strong>gs, database<br />

browsing<br />

Segmentation <strong>of</strong> speech<br />

versus non speech in<br />

automatic speech<br />

recognition tasks<br />

Automatic co<strong>din</strong>g and<br />

content based<br />

audio/vi<strong>de</strong>o retrieval<br />

―Table <strong>of</strong> Content<br />

<strong>de</strong>scription‖ <strong>of</strong> a<br />

multimedia document<br />

Audio content analysis<br />

in vi<strong>de</strong>o parsing<br />

12 MFCC, Short-time energy<br />

Silence ratio, volume std, volume dynamic<br />

range, 4Hz freq, mean and std <strong>of</strong> pitch<br />

difference,<br />

speech, noise ratios, freq. centroid,<br />

bandwidth, energy in 4 sub-bands<br />

Features based on short-time energy,<br />

average ZCR, short-time fundamental<br />

frequency<br />

Mean per-frame entropy and average<br />

probability ―dynamism‖, background-label<br />

energy ratio, phone distribution match—<br />

all <strong>de</strong>rived from posterior probabilities <strong>of</strong><br />

phones in hybrid connectionist-HMM<br />

framework<br />

LSF, differential LSF, measures based on<br />

the ZCR <strong>of</strong> high-pass filtered signal<br />

ZCR-based features, spectral flux,<br />

shorttime energy, cepstrum coefficients,<br />

spectral centroids, ratio <strong>of</strong> the highfrequency<br />

power spectrum, a measure<br />

based on syllabic frequency<br />

High zero-crossing rate ratio (HZCRR),<br />

low short-time energy ratio (LSTER),<br />

Template matching <strong>of</strong><br />

histograms, a tree-based<br />

vector quantizer,<br />

trained to maximize mutual<br />

information<br />

A neural network using the<br />

one-class-in-one network<br />

(OCON) structure<br />

A rule-based heuristic<br />

procedure for the coarse<br />

stage, HMM for the second<br />

stage<br />

Gaussian likelihood ratio<br />

test<br />

KNN classifier and<br />

quadratic Gaussian<br />

classifier (QCG)<br />

Multivariate Gaussian<br />

classifier, neural network<br />

(MLP)<br />

3-step classification:<br />

1. KNN and linear spectral<br />

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56 Adrian Simion, Ștefan Trăușan-Matu<br />

2002 [12] linear spectral<br />

pairs, band periodicity, noise-frame ratio<br />

(NFR)<br />

Ajmera et al.,<br />

2003 [13]<br />

Burred and<br />

Lerch, 2004<br />

[14]<br />

Barbedo and<br />

Lopes, 2006<br />

[15]<br />

Mu˜noz- Exp´<br />

osito et al.,<br />

2006 [16]<br />

Alexandre et<br />

al, 2006 [17]<br />

Automatic transcription<br />

<strong>of</strong> broadcast news<br />

Audio classification<br />

(speech/<br />

music/background<br />

noise), music<br />

classification into genres<br />

Automatic segmentation<br />

for real-time<br />

applications<br />

Intelligent audio co<strong>din</strong>g<br />

system<br />

Speech/music<br />

classification for<br />

musical genre<br />

classification<br />

Averaged entropy measure and<br />

―dynamism‖ estimated at the output <strong>of</strong> a<br />

multilayer perceptron (MLP) trained to<br />

emit posterior probabilities <strong>of</strong> phones.<br />

MLP input: 13 first cepstra <strong>of</strong> a 12th-or<strong>de</strong>r<br />

perceptual linear prediction filter.<br />

Statistical measures <strong>of</strong> short-time frame<br />

features: ZCR, spectral centroid/roll<br />

<strong>of</strong>f/flux,<br />

first 5 MFCCs, audio spectrum<br />

centroid/flatness, harmonic ratio, beat<br />

strength, rhythmic regularity, RMS<br />

energy, time envelope, low energy rate,<br />

loudness<br />

Features based on ZCR, spectral roll <strong>of</strong>f,<br />

loudness and fundamental frequencies<br />

Warped LPC-based spectral centroid<br />

Spectral centroid/roll <strong>of</strong>f, ZCR, short-time<br />

energy, low short time energy ratio<br />

(LSTER), MFCC, voice to-white<br />

pairs-vector quantization<br />

(LSP-VQ)for<br />

speech/nonspeech<br />

discrimination.<br />

2. Heuristic rules for<br />

nonspeech classification<br />

into music/background<br />

noise/silence.<br />

3. Speaker segmentation<br />

2-state HMM with<br />

minimum duration<br />

constraints (threshold free,<br />

unsupervised, no training).<br />

KNN classifier, 3-<br />

component GMM classifier<br />

KNN, self-organizing<br />

maps, MLP neural<br />

networks, linear<br />

combinations<br />

3-component GMM, with<br />

or without fuzzy rulesbased<br />

system<br />

Fisher linear discriminant,<br />

K nearest neighbor<br />

2.1. Digital Audio Signals<br />

When music is recor<strong>de</strong>d, the continuous pressure from the sound wave is<br />

measured using a microphone. These measurements are taken at a regular time<br />

and each measurement is quantized.<br />

Fig. 1. Digital sound representation (time domain):<br />

a. Music is a b. that is sampled… c. and Quantized<br />

continuous signal;… .<br />

Sound can be represented as a sum <strong>of</strong> sinusoids. A signal <strong>of</strong> N samples can be<br />

written as:<br />

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Automatic Computer Music Classification and Segmentation 57<br />

N / 2<br />

( r)<br />

k ( i)<br />

k<br />

x ak<br />

cos(2 ( )) ak<br />

sin(2<br />

( )).<br />

(1)<br />

k0<br />

N<br />

N<br />

The signal can be represented in the frequency domain using the<br />

( y)<br />

( i)<br />

( y)<br />

i<br />

coefficients {( a<br />

1<br />

, a1<br />

),...,( aN<br />

/ 2,<br />

aN<br />

/ 2)}<br />

.<br />

The magnitu<strong>de</strong> and phase <strong>of</strong> the k th frequency component are given by:<br />

X<br />

M<br />

[ k]<br />

( r)<br />

2 ( i)<br />

2<br />

( ak<br />

) ( ak<br />

)<br />

(2)<br />

( i)<br />

ak<br />

X<br />

p[ k]<br />

arctan( )<br />

( r)<br />

(3)<br />

ak<br />

Perceptual studies on human hearing show that the phase information is relatively<br />

unimportant when compared to magnitu<strong>de</strong> information, thus the phase component<br />

during feature extraction is usually ignored. [19]<br />

The Spectral Centroid is another spectral-shape feature that is useful in the<br />

extraction and analysis process. We can see form Table 1 its various uses. The<br />

Spectral Centroid is the center <strong>of</strong> gravity <strong>of</strong> the spectrum and is given by:<br />

N / 2<br />

<br />

X<br />

M<br />

[ k]*<br />

k<br />

k 1<br />

C (4)<br />

N / 2<br />

X [ k]<br />

<br />

k 1<br />

M<br />

The Spectral Centroid can be thought <strong>of</strong> as a measure <strong>of</strong> ‗brightness‘ since songs<br />

are consi<strong>de</strong>r brighter when they have more high frequency components.<br />

2.2. Time-Frequency Domain Transforms<br />

In MIR and sound analysis in general it is common to do transformation between<br />

the time and frequency domains. For this the mathematical apparatus gives us the<br />

real discrete Fourier transform (DFT), the real short-time Fourier transform<br />

(STFT), discrete cosine transform (DCT), discrete wavelet transform (DWT) and<br />

also the gammatone transform (GT).<br />

Music analysis is not concerned with complex transforms, since music is always a<br />

real-valued time series and has only positive frequencies.<br />

Given a signal x with N samples, the basis functions for the DFT will be N/2 sine<br />

waves and N/2 cosine waves that correspond to the previous coefficients.<br />

The projection operator is correlation, which is a measure <strong>of</strong> how similar two time<br />

series are to one another. The coefficients are found by:<br />

( r)<br />

k<br />

ak<br />

x[<br />

i]cos(2 i)<br />

(5)<br />

N<br />

1<br />

2 N<br />

N i0<br />

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58 Adrian Simion, Ștefan Trăușan-Matu<br />

1<br />

( i)<br />

2 N k<br />

ak<br />

x[<br />

i]cos(<br />

2 i)<br />

(6)<br />

N i0<br />

N<br />

The DFT is computed in an efficient manner by the fast Fourier transform FFT.<br />

One drawback <strong>of</strong> both the time series representation and the spectrum<br />

representation is that neither simultaneously represents both time and frequency<br />

information. A time-frequency representation is found using the short-time<br />

Fourier transform (STFT): First, the audio signal is broken up into a series <strong>of</strong><br />

(overlapping) segments. Each segment is multiplied by a window function. The<br />

length <strong>of</strong> the window is called the window size.<br />

Fig. 2. Magnatune apa_ya-apa_ya-14-maani-59-88.wav (time domain).<br />

Fig. 3. Magnatune apa_ya-apa_ya-14-maani-59-88.wav (spectrogram).<br />

Fig 2 and 3 were obtained with a tweaked version <strong>of</strong> the MARSYAS‘s tool<br />

sound2png with the following commands:<br />

./sound2png -m waveform ../audio/magnatune/0/apa_ya-apa_ya-14-maani-59-88.wav<br />

../saveres/magnatunewav.png -ff Adventure.ttf<br />

./sound2png -m spectogram ../audio/magnatune/0/apa_ya-apa_ya-14-maani-59-88.wav<br />

../saveres/magnatunespec.png -ff Adventure.ttf<br />

Another useful transformation is the wavelet transform.<br />

2.3. Mel-Frequency Cepstral Coefficients (MFCC)<br />

The most common set <strong>of</strong> features used in speech recognition and music annotation<br />

systems are the Mel-Frequency Cepstral Coefficients (MFCC). MFCC are shorttime<br />

features that characterize the magnitu<strong>de</strong> spectrum <strong>of</strong> an audio signal. For<br />

each short-time (25 ms) segment, the feature vector is found using the five step<br />

algorithm given in Algorithm 1. The first step is to obtain the magnitu<strong>de</strong> <strong>of</strong> each<br />

frequency component in the frequency domain using the DCT We then take the<br />

log <strong>of</strong> the magnitu<strong>de</strong> since perceptual loudness has been shown to be<br />

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Automatic Computer Music Classification and Segmentation 59<br />

approximately logarithmic. The frequency components are then merged into<br />

40 bins that have been space accor<strong>din</strong>g the Mel-scale.<br />

The Mel-scale is mapping between true frequency and a mo<strong>de</strong>l <strong>of</strong> perceived<br />

frequency that is approximately logarithmic.<br />

Since a time-series <strong>of</strong> these 40-dimensional Mel-frequency vectors will have<br />

highly redundant, we could reduce dimension using PCA.<br />

Instead, the speech community has adopted the discrete cosine transform (DCT),<br />

which approximates PCA but does not require training data, to reduce the<br />

dimensionality to a vector <strong>of</strong> 13 MFCCs. [20]<br />

Algorithm 1. Calculating MFCC Feature Vector<br />

1: Calculate the spectrum using the DFT<br />

2: Take the log <strong>of</strong> the spectrum<br />

3: Apply Mel-scaling and smoothing<br />

4: Decorrelate using the DCT.<br />

3. Problem <strong>de</strong>scription<br />

A common feature that aids record producers to meet the <strong>de</strong>mands <strong>of</strong> the target<br />

audiences, musicologists to study musical influences and music enthusiasts to<br />

summarize their collections is the musical genre i<strong>de</strong>ntification.<br />

The genre concept is inherently subjective because the influences, hierarchy or the<br />

intersection <strong>of</strong> a song to a specific genre isn‘t universally agreed upon.<br />

This point is backed up by a comparison <strong>of</strong> three Internet music provi<strong>de</strong>rs that<br />

found very big differences in the number <strong>of</strong> genres, the words that <strong>de</strong>scribe that<br />

genre, and the structure <strong>of</strong> the genre hierarchies. [18]<br />

Although there are some inconsistencies caused by its subjective nature, the genre<br />

concept has shown interest from the MIR community.<br />

The various papers and works on this subject reflect the authors‘ assumptions<br />

about the genres. Copyright laws prevented authors from establishing a common<br />

database <strong>of</strong> songs, making it difficult to directly compare the results.<br />

4. Experiments <strong>de</strong>scription<br />

The datasets used for training and testing were MAGNATUNE [21] and two<br />

collections that were built in the early stages <strong>of</strong> the MARSYAS [22] framework.<br />

As the ADAMS system is built in a modular form the various tasks (<strong>de</strong>scribed<br />

below) can be automatized and the sound can ―flow‖ through these modules until<br />

the complete analysis is ma<strong>de</strong>.<br />

The ADAMS main directory structure can be seen in the following picture:<br />

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60 Adrian Simion, Ștefan Trăușan-Matu<br />

Fig. 4. ADAMS Main Directory Structure.<br />

The machine learning tasks are done with the WEKA [23] tool, loa<strong>din</strong>g the<br />

compatible arff files produced with the aid <strong>of</strong> MARSYAS.<br />

The chosen OS for these experiments was Mandriva Linux 2011, the compiler<br />

version being ―gcc (GCC) 4.6.1 20110627 (Mandriva)‖.<br />

Extractors that were used:<br />

- BEAT: Beat histogram features<br />

- LPCC: LPC <strong>de</strong>rived Cepstral coefficients<br />

- LSP: Linear Spectral Pairs<br />

- MFCC: Mel-Frequency Cepstral Coefficients<br />

- SCF: Spectral Crest Factor (MPEG-7)<br />

- SFM: Spectral Flatness Measure (MPEG-7)<br />

- SFMSCF: SCF and SFM features<br />

- STFT: Centroid, Roll<strong>of</strong>f, Flux, ZeroCrossings<br />

- STFTMFCC: Centroid, Roll<strong>of</strong>f Flux, ZeroCrossings, Mel-Frequency<br />

Cepstral Coefficients<br />

On every experiment for the specified extractors are also presented the confusion<br />

matrices [24] in or<strong>de</strong>r to have an i<strong>de</strong>a about the actual and the predicted<br />

classifications done by the classification system.<br />

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Automatic Computer Music Classification and Segmentation 61<br />

4.1. Experiment 1: Classification using “Timbral Features”<br />

This experiment uses the following extractors: Time ZeroCrossings, Spectral<br />

Centroid, Flux and Roll<strong>of</strong>f, and Mel-Frequency Cepstral Coefficients (MFCC).<br />

We extract these features with the option – timbral and we also create the file that<br />

will be loa<strong>de</strong>d with the WEKA environment for analysis with the following<br />

command:<br />

./adamsfeature -sv -timbral ../col/all.mf -w ../analysis/alltimbral.arff<br />

Based on experiment the following classifiers were chosen: Bayes Network,<br />

Naive Bayes, Decision Table, Filtered Classifier and NNGE.<br />

The results are shown in the following table:<br />

Table 2. Timbral Features - Classifier Results<br />

Classifier<br />

Mo<strong>de</strong>l<br />

Build<br />

Time(s)<br />

Coorectly<br />

Classified<br />

Incorrectly<br />

Classified<br />

Mean<br />

absolut<br />

error<br />

Root<br />

mean<br />

squared<br />

error<br />

Relative<br />

absolute<br />

error<br />

Root<br />

relative<br />

squared<br />

error<br />

Bayes Network 1.78 62.5% 37.5% 0.0753 0.2648 41.82% 88.28%<br />

Naive Bayes 0.04 55% 45% 0.0902 0.2925 50.09% 97.51%<br />

Decision Table 15.49 51.6% 48.4% 0.1467 0.2599 81.53% 86.64%<br />

Filtered Classifier 4.55 87.8% 12.2% 0.0348 0.1318 19.31% 43.94%<br />

NNGE 10.69 100% 0% 0 0 0 0<br />

Table 2 was build loa<strong>din</strong>g the file alltimbral.arff in WEKA and training the builtin<br />

classifiers<br />

Fig. 5. WEKA Prediction Errors Graph.<br />

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62 Adrian Simion, Ștefan Trăușan-Matu<br />

Fig. 6. Confusion Matrices for Timbral Features Classification<br />

4.2. Experiment 2: Classification using “Spectral Features”<br />

This experiment uses the following extractors: Spectral Centroid, Flux and Roll<br />

<strong>of</strong>f. The feature extraction was done with the following command:<br />

./adamsfeature -sv -spfe ../col/all.mf -w ../analysis/allspectral.arff<br />

Using the same classifiers the results are:<br />

Table 3. Spectral Features - Classifier Results<br />

Classifier<br />

Mo<strong>de</strong>l<br />

Build<br />

Time(s)<br />

Correctly<br />

Classified<br />

Incorrectly<br />

Classified<br />

Mean<br />

absolute<br />

error<br />

Root<br />

mean<br />

squared<br />

error<br />

Relative<br />

absolute<br />

error<br />

Root<br />

relative<br />

squared<br />

error<br />

Bayes Network 1.78 46.5% 53.5% 0.1192 0.2742 66.21% 91.41%<br />

Naive Bayes 0.23 42.5% 57.5% 0.1205 0.2924 66.92% 97.47%<br />

Decision Table 0.72 46.1% 53.9% 0.1491 0.2655 82.82% 88.49%<br />

Filtered Classifier 0.41 63.6% 36.4% 0.099 0.2225 54.98% 74.15%<br />

NNGE 2.02 100% 0% 0 0 0 0<br />

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Automatic Computer Music Classification and Segmentation 63<br />

Fig. 7. Confusion Matrices for Spectral Features Classification<br />

4.3 Experiment 2: Classification using “MFCC”<br />

This experiment uses the Mel-Frequency Cepstral Coefficients extractors. The<br />

feature extraction was done with the following command:<br />

./adamsfeature -sv -mfcc ../col/all.mf -w ../analysis/allmfcc.arff<br />

Table 4. MFCC Features - Classifier Results<br />

Classifier<br />

Mo<strong>de</strong>l<br />

Build<br />

Time(s)<br />

Correctly<br />

Classified<br />

Incorrectly<br />

Classified<br />

Mean<br />

absolute<br />

error<br />

Root<br />

mean<br />

squared<br />

error<br />

Relative<br />

absolute<br />

error<br />

Root<br />

relative<br />

squared<br />

error<br />

Bayes Network 1.23 63.3% 36.7% 0.0764 0.2475 42.42% 82.50%<br />

Naive Bayes 0.22 58.5% 41.5% 0.0847 0.2694 47.07% 89.80%<br />

Decision Table 6.4 49.1% 50.9% 0.1481 0.2638 82.27% 87.94%<br />

Filtered Classifier 0.81 87.1% 12.9% 0.0363 0.1348 20.18% 44.92%<br />

NNGE 3.74 99.8% 0.2% 0.0004 0.02 0.22% 6.66%<br />

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64 Adrian Simion, Ștefan Trăușan-Matu<br />

Fig. 8. Confusion Matrices for MFCC Features Classification<br />

4.4 Experiment 4: Classification using “Zero Crossings”<br />

The feature extraction was done with the following command:<br />

./adamsfeature -sv -zcrs ../col/all.mf -w ../analysis/allzcrs.arff<br />

Table 5. Zero Crossings Features - Classifier Results<br />

Classifier<br />

Mo<strong>de</strong>l<br />

Build<br />

Time(s)<br />

Correctly<br />

Classified<br />

Incorrectly<br />

Classified<br />

Mean<br />

absolute<br />

error<br />

Root<br />

mean<br />

squared<br />

error<br />

Relative<br />

absolute<br />

error<br />

Root<br />

relative<br />

squared<br />

error<br />

Bayes Network 0.09 34.7% 65.3% 0.1437 0.2789 79.83% 92.97%<br />

Naive Bayes 0.01 34.5% 65.5% 0.1441 0.2869 80.06% 95.63%<br />

Decision Table 0.22 42.4% 57.6% 0.1511 0.2691 83.95% 89.71%<br />

Filtered Classifier 0.15 44% 56% 0.1403 0.2649 77.94% 88.24%<br />

NNGE 0.52 99.8% 0.2% 0.0004 0.02 0.22% 6.66%<br />

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Automatic Computer Music Classification and Segmentation 65<br />

Fig. 9. Confusion Matrices for Zero Crossings Features Classification.<br />

4.5 Experiment 5: Classification using “Spectral Flatness Measure”<br />

The feature extraction was done with the following command:<br />

./adamsfeature -sv -sfm ../col/all.mf -w ../analysis/allsfm.arff<br />

Table 6. SFM Features - Classifier Results<br />

Classifier<br />

Mo<strong>de</strong>l<br />

Build<br />

Time(s)<br />

Correctly<br />

Classified<br />

Incorrectly<br />

Classified<br />

Mean<br />

absolute<br />

error<br />

Root<br />

mean<br />

squared<br />

error<br />

Relative<br />

absolute<br />

error<br />

Root<br />

relative<br />

squared<br />

error<br />

Bayes Network 1.78 58.4% 41.6% 0.0838 0.2738 46.53% 91.28%<br />

Naive Bayes 0.15 53.2% 46.8% 0.0935 0.294 51.96% 97.99%<br />

Decision Table 12.35 50.4% 49.6% 0.1472 0.2621 81.78% 87.37%<br />

Filtered Classifier 2.1 83.8% 16.2% 0.045 0.15 25.01% 50.12%<br />

NNGE 9.24 99.8% 0.2% 0.0004 0.02 0.22% 6.66%<br />

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66 Adrian Simion, Ștefan Trăușan-Matu<br />

Conclusions<br />

Fig. 10. Confusion Matrices for Spectral Flatness Measure Features Classification.<br />

Five experiments were conducted for <strong>de</strong>termining the music genre <strong>of</strong> a specific<br />

audio file. The extracted features varied in each experiment in or<strong>de</strong>r to <strong>de</strong>termine<br />

which one was more suited to the dataset used. The five classifiers provi<strong>de</strong>d<br />

different results based on the extracted features and these were put to test with<br />

well known machine learning tools and music analysis frameworks like WEKA<br />

and MARSYAS, and also with an analysis system <strong>de</strong>veloped on top <strong>of</strong> the<br />

MARSYAS framework.<br />

The results show that satisfactory results can be obtained even from the simplistic<br />

approaches as Naïve Bayes classification, but better results were obtained using<br />

more advanced techniques. The fact that the nearest neighbor produced very good<br />

results doesn‘t mean that it will have the same behavior on another dataset.<br />

Improvements on the presented methods can be obtained by testing these methods on<br />

a broa<strong>de</strong>r dataset and <strong>de</strong>termining the intrinsic influences <strong>of</strong> each genre on another.<br />

The conclusions <strong>of</strong> these influences can have a more meaningful sense from the<br />

social point <strong>of</strong> view like blues and its <strong>de</strong>rivatives and we can find very unlikely<br />

results like <strong>de</strong>ath metal having roots in jazz music.<br />

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Automatic Computer Music Classification and Segmentation 67<br />

R E F E R E N C E S<br />

[1] Howes, F. Man Mind and Music. Marin Secker & Warbug LTD., 1948.<br />

[2] Ismir. http://www.ismir.net/ (Visited on 2012/01/23)<br />

[3] Mirex. http://www.music-ir.org/mirex/wiki/MIREX_HOME (Visited on 2012/01/23)<br />

[4] J. Saun<strong>de</strong>rs, Real-time discrimination <strong>of</strong> broadcast speech/music, in Procee<strong>din</strong>gs <strong>of</strong> IEEE<br />

International Conference on Acoustics, Speech, and Signal Processing (ICASSP ‘96), vol. 2, pp. 993–<br />

996, Atlanta, Ga, USA, May 1996.<br />

[5] E. Scheirer and M. Slaney, Construction and evaluation <strong>of</strong> a robust multifeature speech/music<br />

discriminator, in Procee<strong>din</strong>gs <strong>of</strong> the IEEE International Conference on Acoustics, Speech, and Signal<br />

Processing (ICASSP ‘97), vol. 2, pp. 1331–1334, Munich, Germany, April 1997.<br />

[6] J. T. Foote, A similarity measure for automatic audio classification, in Procee<strong>din</strong>gs <strong>of</strong> the AAAI<br />

Spring Symposium on Intelligent Integration and Use <strong>of</strong> Text, Image, Vi<strong>de</strong>o, and Audio Corpora,<br />

Stanford, Calif, USA, March 1997.<br />

[7] Z. Liu, J. Huang, Y. Wang, and I. T. Chen, Audio feature extraction and analysis for scene<br />

classification, in Procee<strong>din</strong>gs <strong>of</strong> the 1st IEEE Workshop on Multimedia Signal Processing (MMSP<br />

‘97), pp. 343–348, Princeton, NJ, USA, June 1997.<br />

[8] T. Zhang and C.-C. J. Kuo, Hierarchical classification <strong>of</strong> audio data for archiving and<br />

retrieving, in Procee<strong>din</strong>gs <strong>of</strong> IEEE International Conference on Acoustics, Speech, and Signal<br />

Processing (ICASSP ‘99), vol. 6, pp. 3001–3004, Phoenix, Ariz, USA, March 1999.<br />

[9] G. Williams and D. P. W. Ellis, Speech/music discrimination based on posterior probability<br />

features, in Procee<strong>din</strong>gs <strong>of</strong> the 6th European Conference on Speech Communication and Technology<br />

(EUROSPEECH ‘99), pp. 687–690, Budapest, Hungary, September 1999.<br />

[10] K. El-Maleh, M. Klein, G. Petrucci, and P. Kabal, Speech/music discrimination for multimedia<br />

applications, in Procee<strong>din</strong>gs <strong>of</strong> IEEE International Conference on Acoustics, Speech, and Signal<br />

Processing (ICASSP ‘00), vol. 6, pp. 2445–2448, Istanbul, Turkey, June 2000.<br />

[11] A. Bugatti, A. Flammini, and P. Migliorati, Audio classification in speech and music: a<br />

comparison between a statistical and a neural approach, EURASIP Journal on Applied Signal<br />

Processing, vol. 2002, no. 4, pp. 372–378, 2002.<br />

[12] L. Lu, H.-J. Zhang, and H. Jiang, Content analysis for audio classification and segmentation,<br />

IEEE Transactions on Speech and Audio Processing, vol. 10, no. 7, pp. 504–516, 2002.<br />

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68 Adrian Simion, Ștefan Trăușan-Matu<br />

[13] J. Ajmera, I. McCowan, and H. Bourlard, Speech/music segmentation using entropy and<br />

dynamism features in a HMM classification framework, Speech Communication, vol. 40, no. 3, pp.<br />

351-363, 2003.<br />

[14] J. J. Burred and A. Lerch, Hierarchical automatic audio signal classification, Journal <strong>of</strong> the<br />

Audio Engineering Society, vol. 52, no. 7-8, pp. 724–739, 2004.<br />

[15] J. G. A. Barbedo and A. Lopes, A robust and computationally efficient speech/music<br />

discriminator, Journal <strong>of</strong> the Audio Engineering Society, vol. 54, no. 7-8, pp. 571–588, 2006.<br />

[16] J. E. Mu˜noz-Exp ´ osito, S. G. Gal´an, N. R. Reyes, P. V. Can<strong>de</strong>as, and F. R. Pe˜na, A fuzzy<br />

rules-based speech/music discrimination approach for intelligent audio co<strong>din</strong>g over the Internet, in<br />

Procee<strong>din</strong>gs <strong>of</strong> the 120th Audio Engineering Society Convention (AES ‘06), Paris, France, May 2006,<br />

paper number 6676.<br />

[17] E. Alexandre, M. Rosa, L. Caudra, and R. Gil-Pita, Application <strong>of</strong> Fisher linear discriminant<br />

analysis to speech/music classification, in Procee<strong>din</strong>gs <strong>of</strong> the 120th Audio Engineering Society<br />

Convention (AES ‘06), Paris, France, May 2006, paper number 6678<br />

[18] F. Pachet and D. Cazaly, A taxonomy <strong>of</strong> musical genres, RIAO ‘00: Content-Based Multimedia<br />

Information Access, 2000.<br />

[19] B. Logan, Mel-Frequency Cepstral Coefficients for music mo<strong>de</strong>ling, ISMIR ‘00: International<br />

Symposium on Music Information Retrieval, 2000.<br />

[20] D. Turnbull, Automatic music annotation, Department <strong>of</strong> Computer Science, UC San Diego,<br />

2005.<br />

[21] Mangatune. http://tagatune.org/Magnatagatune.html (Visited on 2012/01/23).<br />

[22] MARSYAS. http://marsyas.info/ (Visited on 2012/01/23).<br />

[23] WEKA. http://www.cs.waikato.ac.nz/ml/weka/ (Visited on 2012/01/23).<br />

[24] http://www2.cs.uregina.ca/~hamilton/courses/831/notes/confusion_matrix/confusion_matrix.<br />

html.<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066-8562 Volume 5, Number 1/2012 69<br />

POLYMERIC PRESSURE SENSORS: A CONCEPTUAL VIEW<br />

Cornel COBIANU 1* and Bogdan SERBAN 1<br />

Abstract. In the first part <strong>of</strong> this paper, we present a review <strong>of</strong> the piezoresistive pressure<br />

sensors based on polymeric thick films <strong>de</strong>posited on rigid and flexible diaphragm. The<br />

study <strong>of</strong> the state <strong>of</strong> the art has shown the performances <strong>of</strong> this technology, where<br />

maximum sensitivity is obtained on thin flexible diaphragm for a gauge factor <strong>of</strong> about<br />

10, in a pressure range <strong>of</strong> 05 kPa. The present challenges come from the high<br />

temperature coefficient <strong>of</strong> the resistance <strong>of</strong> about 500 ppm/C, and the long temperature<br />

drifts <strong>of</strong> about (0.52)%, which may require improved repeatability <strong>of</strong> fabrication<br />

technology and advanced differential signal processing techniques for the market<br />

acceptance. In the second part <strong>of</strong> the paper, we present our novel concepts for the<br />

realization <strong>of</strong> the piezoresistive pressure sensors. The first concept consists in the surface<br />

modification <strong>of</strong> the organic substrate by ion implantation <strong>of</strong> nitrogen and phosphorus<br />

species for creating piezoresistive behavior and high electrical conductivity <strong>of</strong> organic<br />

piezoresistors. The second concept consists in the novel chemical synthesis route <strong>of</strong><br />

organic thin film by doping the polyaniline with large molecules <strong>of</strong> p-sulfonated<br />

calix[n]arene (n =4, 6, 8), sulfonated crown ethers, in the liquid state. Addition <strong>of</strong> the<br />

metal nanoparticles to the previous homogeneous solution can further increase the<br />

piezoresistive factor. Other new features <strong>of</strong> our second concept come from the direct<br />

printing from solution <strong>of</strong> the above piezoresistive organic thin films, as well as metallic<br />

films interconnecting the piezoresistors, and finally the monolithic fabrication <strong>of</strong> the<br />

sensor rim and diaphragm by plastic injection mol<strong>din</strong>g, where the pressure diaphragm<br />

could be as thin as 75 micrometers.<br />

Keywords: piezoresistive organic films, polymeric thick film, pressure sensors, metal<br />

Nanoparticples, p-sulfonated calix[n]arene, sulfonated crown ethers<br />

1. Introduction<br />

Pressure monitoring is an important parameter in the control <strong>of</strong> a large diversity <strong>of</strong><br />

industrial processes and medical applications. Pressure can be measured by<br />

mechanical <strong>de</strong>vices, as well as electro-mechanical and electro-optical instruments.<br />

The measurement <strong>of</strong> the pressure <strong>of</strong> a fluid by pure mechanical principle is based<br />

on the presence <strong>of</strong> an elastic diaphragm fixed at one end, which is moving its free<br />

end as a result <strong>of</strong> pressure variation, and its position change is indicated by a<br />

needle connected to the free end, and which is thus rotating with respect to its zero<br />

position (Fig. 1).<br />

This principle is used for the pressure measurement on gas/liquids pipelines,<br />

where pressure manometers based on Bourdon tubes are still in place, today.<br />

1 Honeywell Romania, Sensors and Wireless Laboratory, Bucharest, Romania.<br />

*Member <strong>of</strong> Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, cornel.cobianu@honeywell.com.<br />

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70 Cornel Cobianu, Bogdan Serban<br />

In other cases, the elastic diaphragm is fixed at both ends, and this is <strong>de</strong>flecting in<br />

the central part as a result <strong>of</strong> pressure change (Fig. 2). Such <strong>de</strong>flection is creating<br />

strain in the diaphragm, and its value can be also used for the pressure<br />

measurement, in the so called strain gauges. These <strong>de</strong>flecting diaphragms have<br />

opened the way for the electro-mechanical principles <strong>of</strong> pressure measurement.<br />

Fig. 1. Schematic picture <strong>of</strong> a Bourdon<br />

tube used for a pressure manometer.<br />

Fig. 2. Pressure diaphragm flexing<br />

un<strong>de</strong>r applied external pressure.<br />

Historically speaking, in 1856 Lord Kelvin has discovered that the electrical<br />

conductor can change its electrical resistance, when it is strained due to an<br />

external applied force. Thus, he can be credited with the discovery <strong>of</strong> the<br />

piezoresistive effect in metals, which was then used in metallic strain gauge<br />

<strong>de</strong>vices for multiple applications (strain, torque, force) inclu<strong>din</strong>g pressure sensing.<br />

Later, the piezoresistive effect was <strong>de</strong>fined as a change in the electrical resistivity<br />

<strong>of</strong> a material as a function <strong>of</strong> the externally applied stress on it. Now, it is<br />

generally agreed that the discovery <strong>of</strong> piezoresistive effect is at the origin <strong>of</strong> the<br />

most <strong>of</strong> electric sensors for mechanical measurands <strong>de</strong>fined as <strong>de</strong>vices able to<br />

convert a non-electrical signal (like fluid) pressure into an electrical signal (like<br />

voltage). The silicon technology followed by the micro-electro-mechanical system<br />

(MEMS) technology have used all these principles for the miniaturization <strong>of</strong> the<br />

existing macroscopic <strong>de</strong>vices and sensors.<br />

The impetuous <strong>de</strong>velopment <strong>of</strong> the MEMS technology was foun<strong>de</strong>d on two<br />

important technical pillars, consisting <strong>of</strong> well-established integrated circuit (IC)<br />

infrastructure and excellent operation <strong>of</strong> the macroscopic principles at the<br />

micrometer scale. A convincing <strong>de</strong>monstration <strong>of</strong> this successful approach is<br />

coming from microsystems for pressure measurement, where the well-known<br />

principle <strong>of</strong> macroscopic diaphragm movement as a function <strong>of</strong> pressure has been<br />

transferred to microtechnology scale with very good results.<br />

The era <strong>of</strong> miniaturized pressure sensors has been triggered by the discovery <strong>of</strong><br />

the piezoresistive effect in silicon and germanium, in 1954 by Charles Smith [1].<br />

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Polymeric Pressure Sensors:<br />

A Conceptual View 71<br />

The time interval from piezoresistance discovery to the first associated<br />

commercial product was short, as in 1959, Kulite was already <strong>de</strong>livering the first<br />

silicon strain-gauges bon<strong>de</strong>d on a metal diaphragm. During sensor operation, the<br />

metal diaphragm is elastically <strong>de</strong>flecting due to the applied pressure, and a tensile<br />

stress is <strong>de</strong>veloped in the central region <strong>of</strong> the diaphragm, while a compressive<br />

stress is <strong>de</strong>veloped at the periphery <strong>of</strong> the diaphragm (Fig. 2.).<br />

Such a stress is transmitted to the strain gauge, which “is feeling” it by the wellknown<br />

stress-strain correlation, and a change in the resistance is obtained due to<br />

the piezoresistive effect, which is thus an indication <strong>of</strong> the pressure to be<br />

measured. In the presence <strong>of</strong> an external pressure, a piezoresistor located on the<br />

central part <strong>of</strong> the diaphragm from Fig. 2. is exposed to tensile stress and its<br />

resistance value is increasing, while a piezoresistor located at the periphery <strong>of</strong> the<br />

diaphragm, near the edge, is exposed to compressive stress and its resistance value<br />

is <strong>de</strong>creasing with respect to the value specific to zero stress. For an accurate<br />

pressure measurement, where the ageing effects in the piezoresistors, as well as<br />

external temperature variations to be compensated, four piezoresistors are located<br />

in the arms <strong>of</strong> a Wheatstone bridge, and thus obtaining a differential sensing<br />

configuration for the signal conditioning.<br />

Using such an approach, at the beginning <strong>of</strong> 1970‟s, IBM has proven the<br />

operation <strong>of</strong> the first piezoresistive pressure sensor with silicon diaphragm, while<br />

the first commercial “all-silicon” pressure sensor was <strong>de</strong>livered in 1974 [2].<br />

The piezoresistive effect was measured in doped silicon resistors, which were<br />

located in well-<strong>de</strong>fined regions <strong>of</strong> the diaphragm, as <strong>de</strong>scribed above. The<br />

excellent elastic properties <strong>of</strong> silicon diaphragm, combined with the fact that the<br />

silicon piezoresistor is obtained intrinsically in the diaphragm, without any need<br />

<strong>of</strong> strain gauge bon<strong>din</strong>g to silicon diaphragm can explain the excellent<br />

performance <strong>of</strong> silicon MEMS pressure sensors. Thus, the MEMS silicon<br />

technology has proven its capability to generate commercial products, where thin<br />

silicon diaphragms have been used from very beginning in medical application for<br />

measuring blood pressure.<br />

In parallel with silicon MEMS technology, which has brought to the market the<br />

first miniaturized microsystems, sensors and actuators, like pressure sensors,<br />

accelerometers, inkjet nozzles for thermal inkjet technologies and thus predicting<br />

its long-term innovation capabilities, other sensing technologies were emerging,<br />

which were targeting mechanical sensing applications (pressure torque, force)<br />

based on other than silicon materials and substrates. It is the case <strong>of</strong> thick film<br />

technologies which have found their niche sensing applications.<br />

In this paper, we shall briefly present polymeric film technologies for pressure<br />

sensing applications. At the beginning <strong>of</strong> the study, the state <strong>of</strong> the art for the<br />

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72 Cornel Cobianu, Bogdan Serban<br />

piezoresistive polymeric thick films will be shown, where such materials are<br />

<strong>de</strong>posited on diaphragms ma<strong>de</strong> <strong>of</strong> glass, alumina, or even flexible substrates, and<br />

their pressure sensing properties are <strong>de</strong>scribed [3-6].<br />

Finally, our concepts for new polymeric pressure sensors, inclu<strong>din</strong>g “all-organic”<br />

technologies will be shown. Here, firstly, we present a novel pressure sensing<br />

concept, where the plastic substrate will receive electrical conductivity and<br />

piezoresistivity properties on well-<strong>de</strong>fined regions <strong>of</strong> the organic diaphragm by<br />

using IC specific technology like ion implantation [7]. Then, another novel<br />

concept for “all-plastic” pressure sensor is <strong>de</strong>scribed where chemical synthesis for<br />

the preparation <strong>of</strong> new organic thin films with enhanced electrical conductivity is<br />

shown. This piezoresistive pressure sensor is ma<strong>de</strong> by additive, maskless direct<br />

printing <strong>of</strong> the organic films in well-<strong>de</strong>fined positions <strong>of</strong> plastic diaphragm, which<br />

is obtained by injection mol<strong>din</strong>g [8].<br />

2. Piezoresistive pressure sensors based on thick film resistors<br />

The operation principle <strong>of</strong> the piezoresistive mechanical sensors based on thick<br />

films is similar to that <strong>de</strong>scribed for silicon sensors, but the diaphragm and the<br />

piezoresistor are ma<strong>de</strong> <strong>of</strong> different materials. For the evaluation <strong>of</strong> different<br />

piezoresistive materials, the gauge factor is used, and this is equal to the ratio<br />

between the relative variation <strong>of</strong> the resistance (∆R/R) and the relative variation <strong>of</strong><br />

the resistor length (or the strain (∆/)). The piezoresistive behavior in thick<br />

resistive layers was systematically investigated by using commercial ruthenate<br />

thick films from Dupont [9]. The thick films were <strong>de</strong>posited on alumina substrate<br />

as a gel <strong>of</strong> high viscosity by screen printing technology, and then fired at high<br />

temperatures, around 850-950 o C, for obtaining thick solid layers. The gauge<br />

factor for these ruthenate thick films was in the range <strong>of</strong> 11-14, being weakly<br />

<strong>de</strong>pen<strong>de</strong>nt on the strain direction.<br />

Such piezoresistive thick films have a gauge factor which is higher than that <strong>of</strong> the<br />

metal strain gauge (1.8-4.5), and much smaller than that <strong>of</strong> semiconductors (40-<br />

200) [10]. The temperature coefficient <strong>of</strong> these thick ruthenate film piezoresistor<br />

(TCR) was about 100 ppm/ o C, while the temperature coefficient <strong>of</strong> the gauge<br />

factor (TCGF) was smaller than 500 ppm/ o C.<br />

These values can be compared with the similar ones <strong>of</strong> the metal wire strain<br />

gauges, where the TCR has a large range <strong>of</strong> variation (20-4000) ppm/ o C, and<br />

TCGF is in the range 20-100 ppm/ o C [9]. Unfortunately, such high temperature<br />

technology is restricting the type <strong>of</strong> substrate to be used to only ceramics, and is<br />

increasing the cost <strong>of</strong> processing.<br />

As a low temperature alternative to the well-established ruthenate thick film<br />

piezoresistive technology presented above, the pressure sensor based on<br />

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Polymeric Pressure Sensors:<br />

A Conceptual View 73<br />

polymeric thick film resistors was proposed at the beginning <strong>of</strong> the ‟90 exploiting<br />

the piezoresistive effect in such organic layers, which can tolerate processing<br />

temperatures not higher than 150-300 o C [ 3].<br />

The thick film composition consists <strong>of</strong> an organic polymer matrix, like a<br />

polyimi<strong>de</strong>, which is loa<strong>de</strong>d with carbon for obtaining the resistive and<br />

piezoresistive behavior. The sensing diaphragm is ma<strong>de</strong> <strong>of</strong> different rigid<br />

materials like, alumina, glass-reinforced epoxy laminate (FR 4), or even a flexible<br />

substrate [4].<br />

For the realization <strong>of</strong> the planar piezoresistor, initially, the metallic electro<strong>de</strong>s<br />

were <strong>de</strong>posited and patterned on the substrate. Then, the <strong>de</strong>position <strong>of</strong> the<br />

polymeric thick films on the rigid substrate, like alumina, glass, or FR 4 is ma<strong>de</strong><br />

by screen printing technology, followed by thermal consolidation process at low<br />

temperatures, below 300 o C. These planar polymeric thick films based polymeric<br />

piezoresistors have a gauge factor <strong>of</strong> about 10, which is rather similar to the value<br />

obtained for ruthenate thick films, but the TCR is equal to +/ 500 ppm/ o C, which<br />

is much higher with respect to the value obtained for ruthenate material<br />

(100 ppm/ o C).<br />

In the case <strong>of</strong> a “sandwich” piezoresistor configuration, when the polymeric thick<br />

film is sandwiched (on the z direction) between two electro<strong>de</strong>s, with the first<br />

electro<strong>de</strong> <strong>de</strong>posited on the substrate and the second electro<strong>de</strong> <strong>de</strong>posited on the<br />

polymeric thick film, the gauge factor has reached a much higher value <strong>of</strong> about<br />

80 [5]. In addition, these sandwich polymeric piezoresistive pressure sensors have<br />

shown a very high value <strong>of</strong> the TCR, <strong>of</strong> about 2200 ppm/ o C, which may be<br />

more difficult to compensate, even in Wheatstone configuration, due to existing<br />

mismatches between the TCR <strong>of</strong> different piezoresistors.<br />

Also, poorer reproducibility <strong>of</strong> sandwich sensor with respect to planar ones was<br />

obtained.<br />

When such polymeric thick films were <strong>de</strong>posited on flexible substrates, having<br />

much lower thickness with respect to the rigid one, the sensitivity <strong>of</strong> the planar<br />

polymeric thick film pressure sensors has increased <strong>of</strong> about 6 times, but, in our<br />

opinion, this result should be correlated only with the pressure diaphragm<br />

properties (thickness and Young module) and not to sensing layer, itself. Such<br />

thick films polymeric planar pressure sensors on rigid substrate are working in the<br />

temperature range from 0 to 75 o C, and their linear response was obtained for a<br />

pressure range from 0 to 10 6 Pa.<br />

Typical linearity plots <strong>of</strong> the planar polymeric thick film <strong>de</strong>posited on alumina<br />

substrates have shown a non-linearity <strong>of</strong> about 3% in the range [0; +500]<br />

microstrains (1 microstrain means a dilation/shrinkage <strong>of</strong> 1 micrometer <strong>of</strong><br />

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74 Cornel Cobianu, Bogdan Serban<br />

material having a length <strong>of</strong> 1 meter), while the sandwiched piezoresistor have had<br />

a non-linearity <strong>of</strong> 14% in the same strain range [5]. One <strong>of</strong> the biggest drawbacks<br />

<strong>of</strong> such polymeric pressure sensors is the long-term drift, equal to about 0.5-2 %,<br />

and which was estimated by the sensor output drift after an accelerated ageing test<br />

at 1000 o C and 85 o C.<br />

This behavior should be correlated to the specific ageing mechanisms <strong>of</strong> the<br />

organic materials. The „challenging‟ temperature behavior <strong>of</strong> these polymeric<br />

pressure sensors followed by their relative high drifts due to material ageing can<br />

be partially solved by <strong>de</strong>sign <strong>of</strong> the diaphragm (thickness and Young modulus <strong>of</strong><br />

organic substrate) as shown in [3,4] and by means <strong>of</strong> Wheatstone bridge-based<br />

differential signal conditioning.<br />

Therefore, much work should be <strong>de</strong>voted here, but such polymeric sensors are the<br />

best candidate for low cost disposable pressure sensors for applications where the<br />

accuracy is not critical.<br />

3. Piezoresistive pressure sensors based on surface modified polymeric<br />

diaphragm<br />

Flexible electronics (flex circuits), where the “traditional” silicon integrated<br />

circuits are placed by surface mounting technologies on a flexible plastic substrate<br />

is rapidly advancing in many market applications, from portable vi<strong>de</strong>o camera to<br />

solar cell [11].<br />

For these flex circuits, the metallic interconnections between different integrated<br />

circuits are ma<strong>de</strong> by standard photolithographic techniques. In parallel, an “allorganic”<br />

electronics is emerging where the semiconductor <strong>de</strong>vices like organic<br />

light emitting dio<strong>de</strong>s (OLED) and organic field emission transistor (OFET) are<br />

manufactured in the body <strong>of</strong> the organic semiconductor materials [12]. In this<br />

context, the sensing domain is going to add new capabilities to the rigid and<br />

flexible organic electronics. On this i<strong>de</strong>a, recently, we have proposed a concept<br />

for pressure sensors where a polymeric pressure diaphragm is surface modified in<br />

or<strong>de</strong>r to obtain selectively piezoresistive effect [7].<br />

The novelty <strong>of</strong> our approach comes from the technology <strong>of</strong> the piezoresistor<br />

realization, where we have applied ion implantation technique for the local<br />

realization <strong>of</strong> the piezoresistivity and electrical conduction enhancement, as it will<br />

be <strong>de</strong>scribed below. In Fig. 3, we show a cross section view <strong>of</strong> “an-all plastic”<br />

piezoresistive pressure sensor, before packaging, where the substrate and the<br />

diaphragm come from the same starting rigid plastic material, which could be a<br />

polyimi<strong>de</strong>, like Kapton from Dupont or liquid crystal polymer. Alternatively,<br />

polystyrene-co-acrylonitrile (SAN) 80/20 could be used. Such organic polymers<br />

are dielectric materials, which have a very high electrical resistivity, and therefore<br />

they cannot be used “as they are” for reaching the inten<strong>de</strong>d function.<br />

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Polymeric Pressure Sensors:<br />

A Conceptual View 75<br />

Fig. 3. Schematic <strong>of</strong> a pressure sensor with<br />

diaphragm obtained by etching back si<strong>de</strong> <strong>of</strong> the<br />

substrate and piezoresistor fabricated by ion<br />

implantation.<br />

Fig. 4. Pressure with plastic diaphragm bon<strong>de</strong>d<br />

by adhesive to glass.<br />

However, it was already shown in the literature that the ion implantation can<br />

dramatically increase the electrical conduction <strong>of</strong> these plastic materials [13].<br />

Therefore, we have proposed to perform a high dose implantation <strong>of</strong> the nitrogen<br />

species, in well-<strong>de</strong>fined regions <strong>of</strong> the diaphragm for the generation <strong>of</strong> the<br />

piezoresistive regions. This process was followed by a phosphorus ion<br />

implantation in the same region for further enhancement <strong>of</strong> the electrical<br />

conductivity <strong>of</strong> the piezoresistive regions.<br />

For generating such electrical and piezoelectrical properties selectively, in the<br />

organic diaphragm, standard IC photo-lithographical processes can be used. This is<br />

possible due to the chemical resistance <strong>of</strong> these rigid plastic materials to the<br />

solvents and the other solutions used to remove the photoresist, at the end <strong>of</strong> the ion<br />

implantation processes. Subsequently, the electrical contacts to the piezoresistors<br />

are done by IC technology processes like electron-gun physical vapor <strong>de</strong>position,<br />

where, for example, a thin film combination like chromium/gold can be used.<br />

Chromium is assuring the adherence <strong>of</strong> the gold layer to the plastic substrate and<br />

ion-implanted regions <strong>of</strong> the piezoresistors.<br />

For the realization <strong>of</strong> the diaphragm in the starting plastic material, the back-si<strong>de</strong><br />

etching <strong>of</strong> the substrate is performed by plasma techniques, like reactive ion<br />

etching (RIE). The realization <strong>of</strong> such pressure diaphragms from Fig. 3. is<br />

possible by metal masking <strong>of</strong> the entire front si<strong>de</strong>, and <strong>of</strong> selective regions <strong>of</strong> back<br />

si<strong>de</strong> regions <strong>of</strong> the substrate, which should survive after <strong>de</strong>ep etching and<br />

subsequently form what is called the rim <strong>of</strong> the pressure sensor. The thickness <strong>of</strong><br />

the pressure diaphragm is <strong>de</strong>termined by the pressure range nee<strong>de</strong>d to be<br />

measured and the important requirement that the <strong>de</strong>flection <strong>of</strong> the pressure<br />

diaphragm un<strong>de</strong>r external pressure to be in the elasticity domain <strong>of</strong> that material.<br />

Such <strong>de</strong>sign conditions are preserving the linearity <strong>of</strong> the sensor response and also<br />

minimizing the hysteresis and long-term drifts <strong>of</strong> the sensors.<br />

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76 Cornel Cobianu, Bogdan Serban<br />

In other applications, it may be useful to use a glass substrate and a plastic diaphragm<br />

which can be bon<strong>de</strong>d together for <strong>de</strong>fining the pressure sensor. Such an approach is<br />

also possible within the above concept, where initially a plastic foil (similar to the<br />

silicon wafer from the point <strong>of</strong> view <strong>of</strong> batch processing) <strong>of</strong> the thickness required by<br />

the pressure sensing application is processed, as presented above, but, in this case<br />

there is no need for the back si<strong>de</strong> etching, as the entire thickness will play the role <strong>of</strong><br />

the diaphragm. In this case, which is shown in Fig. 4., micromachining <strong>of</strong> the glass<br />

substrate is nee<strong>de</strong>d for the realization <strong>of</strong> the rim <strong>of</strong> the sensor, which is also allowing<br />

the access <strong>of</strong> the fluid pressure (air, liquid) to the pressure diaphragm. Glass MEMS<br />

is a well-established batch technology for sensor applications, and also for sensor<br />

packaging, in general.<br />

In this case, the key process is glass drilling at the “wafer” level for the sensor rim<br />

realization, and this can be done by either wet etching in HF based solutions, or<br />

by RIE or even laser drilling. The signal conditioning techniques are “standard”<br />

consisting in Wheatstone bridge, which will be <strong>de</strong>scribed in more <strong>de</strong>tails, in the<br />

next section.<br />

4. Low cost “all-plastic” piezoresistive pressure sensors<br />

In different industrial domains, there is a strong <strong>de</strong>mand for disposable, low cost<br />

pressure sensors. In such cases, the silicon technology may still be expensive,<br />

consi<strong>de</strong>ring the cost <strong>of</strong> clean room processes, and <strong>of</strong> the monocrystalline silicon<br />

substrate itself.<br />

Fig. 5a. Top view <strong>of</strong> the low cost pressure sensor<br />

ma<strong>de</strong> by plasting mol<strong>din</strong>g and direct printing <strong>of</strong> organic piezoresistive layer.<br />

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Polymeric Pressure Sensors:<br />

A Conceptual View 77<br />

Fig. 5b. Cross section view through 2A-2A axis.<br />

For such applications, where even the photolithographical processing should be<br />

avoi<strong>de</strong>d, we have <strong>de</strong>veloped a concept for a simple technology based on plastic<br />

injection mol<strong>din</strong>g <strong>of</strong> the sensor rim and pressure diaphragm in conjunction with<br />

mask-less, direct printing methods for the <strong>de</strong>position <strong>of</strong> the metal, and novel<br />

organic piezoresistive layers [8].<br />

In Fig. 5. a), we show a top view <strong>of</strong> the pressure sensor based on four<br />

piezoresistors, R 1 -R 4 , all <strong>of</strong> them being located in well-<strong>de</strong>fined positions <strong>of</strong> the<br />

mol<strong>de</strong>d plastic diaphragm, while in Fig. 5. b) we show a cross section view<br />

through the central region <strong>of</strong> the pressure diaphragm.<br />

These piezoresistors are electrically interconnected in a Wheatstone bridge, as<br />

shown in Fig. 6. In the absence <strong>of</strong> an external pressure, all four piezoresistors<br />

have the same value <strong>of</strong> the resistance, and the output voltage <strong>of</strong> the Wheatstone<br />

bridge is equal to zero.<br />

In or<strong>de</strong>r to obtain this zero voltage, two potentiometers are also connected to the<br />

Wheatstone bridge, as in Fig. 5. a) and Fig. 6.<br />

In the presence <strong>of</strong> an external pressure, the piezoresistors R 1 and R 3 , which are<br />

positioned in the central region <strong>of</strong> the diaphragm, are exposed to tensile stress,<br />

while R 2 and R 4 , which are located at the periphery <strong>of</strong> the diaphragm are exposed<br />

to the compressive stress.<br />

The variation <strong>of</strong> the piezoresistance as a function <strong>of</strong> pressure can be written as<br />

follows:<br />

R 1 = R o (1 + x)<br />

R 2 = R o (1 x)<br />

R 3 = R o (1 + x)<br />

R 4 = R o (1 x)<br />

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78 Cornel Cobianu, Bogdan Serban<br />

where, R o is the resistance value <strong>of</strong> the piezoresistor at the reference pressure, while<br />

x = G*ε, where G is the gauge factor <strong>of</strong> piezoresistance, and ε is relative <strong>de</strong>formation<br />

<strong>of</strong> the length <strong>of</strong> the piezoresistor, ε =∆/ [10].<br />

Fig. 6. Wheatstone bridge with four piezoresistors for maximum pressure sensitivity.<br />

As mentioned above, the novel aspects <strong>of</strong> the pressure sensor realization come<br />

from the new organic piezoresistive materials, the maskless method for film<br />

resistor <strong>de</strong>position, and as well as the cheap technology proposed for the plastic<br />

diaphragm realization.<br />

For the realization <strong>of</strong> the piezoresistive films, we are consi<strong>de</strong>ring more chemical<br />

synthesis routes, which are aiming an increased electrical conductivity and<br />

piezoresistivity <strong>of</strong> the organic layer. In the case <strong>of</strong> an all-organic piezoresistive<br />

layer, for example, we suggest starting with polyaniline and doping it with large<br />

molecules like p-sulfonato-calix[n]arenes (n = 4, 6, 8), p-sulfonatedcalix[n]arenes<br />

(n = 4, 6, 8), tosylates, carboxylic acids <strong>of</strong> calix[n]arenes<br />

(n = 4, 6, 8), sulfonated crown ethers, sulfonated cyclo<strong>de</strong>xtrines, carboxylic acid<br />

nanotubes, or carboxylic acid <strong>of</strong> fullerenes.<br />

All these compounds can be dissolved in water and other solvents. They can<br />

generate π-stacking interactions with polyanilines and thus contributing to the<br />

increase <strong>of</strong> electrical conductivity <strong>of</strong> the polymeric film.<br />

In Fig. 7. we show the chemical formulae <strong>of</strong> the p-sulfonated-calix[n]arene for<br />

n = 4, 6, 8, while in Fig. 8., we show the reaction for doping the aniline by<br />

p-sulfonated calix[4]arene. The synthesis <strong>of</strong> a soluble conducting polymer can be<br />

as follows. One can start with aniline substituted with an o-methoxy group and an<br />

o-ethoxy group in equimolar amounts which can be polymerized by combining<br />

with hydrogen peroxi<strong>de</strong>, in aqueous solution. The dopant can be p-sulfonated<br />

calix[n]arenes (n = 4, 6, 8), tosylates, carboxylic acids <strong>of</strong> calix[n]arenes (n =<br />

4, 6, 8), or sulfonated crown ethers [14].<br />

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Polymeric Pressure Sensors:<br />

A Conceptual View 79<br />

SO 3 H<br />

SO 3 H<br />

SO 3 H<br />

CH 2<br />

OH 4<br />

OH<br />

CH 2<br />

6<br />

CH 2<br />

OH 8<br />

Fig. 7. Chemical formula <strong>of</strong> p-sulfonated calix[n]arene, where n = 4, 6, 8.<br />

Fig. 8. Synthesis <strong>of</strong> doped polyaniline; HA stands for p-sulfonated calix [4]arene.<br />

as <strong>de</strong>scribed above. If the electrical and piezoresistive behavior <strong>of</strong> the all-organic<br />

polymer film should be further increased, then, metal nanoparticles may be ad<strong>de</strong>d<br />

to the above polymeric sol, creating thus a heterogeneous inorganic-organic<br />

mixture in the liquid state, which will be further used for the direct printing<br />

method to be <strong>de</strong>scribed below. Thus, an efficient increase <strong>of</strong> the gauge factor <strong>of</strong><br />

the piezoresistors is expected by the addition <strong>of</strong> metal nanoparticles to the liquid<br />

phase <strong>of</strong> the initial pure organic solution.<br />

Fig. 9. Schematics <strong>of</strong> the direct printing method for the maskless preparation <strong>of</strong> solid films.<br />

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80 Cornel Cobianu, Bogdan Serban<br />

In Fig. 9., we show a schematic <strong>of</strong> direct printing apparatus. More data about this<br />

additive <strong>de</strong>position method can be found elsewhere [15]. Specific to this direct<br />

printing method is the formation <strong>of</strong> the liquid precursor <strong>of</strong> the future solid film, by<br />

any chemical syntheses routes, which is then <strong>de</strong>posited in the right location <strong>of</strong> the<br />

substrate by a moving nozzle, while its “travel” above the substrate is computercontrolled.<br />

If we go into more <strong>de</strong>tails, as can be seen in Fig. 8., a gas flow is used<br />

to carry the liquid phase <strong>of</strong> the “atomized” <strong>de</strong>position material to a nozzle, which<br />

is printing the liquid state on the substrate for the realization the pattern <strong>of</strong> the<br />

future solid film. After printing, the “gelly” layers are dried and thermally<br />

consolidated at the temperatures allowed by the organic materials, so that their<br />

chemical properties to be preserved. The advantage <strong>of</strong> this <strong>de</strong>position method is<br />

that the solid film is printed from the very beginning in the right position and<br />

pattern, and there is no need for additional photolithographic and etching process<br />

for the layer <strong>de</strong>lineation. Un<strong>de</strong>r such conditions, there is no loss <strong>of</strong> material and<br />

many technological steps are eliminated.<br />

By this additive technology we can <strong>de</strong>posit not only the polymeric films as<br />

<strong>de</strong>scribed above, but also the metallic films used to interconnect electrically the<br />

piezoresistors from Figs. 5 and 6. For these metallic conductors, one can use<br />

organic conductors, or silver based pastes, which have a low resistivity and do not<br />

introduce parasitic resistances to the Wheatstone bridge.<br />

Finally, a novel aspect <strong>of</strong> our concept is the monolithic realization <strong>of</strong> the sensor<br />

rim and pressure diaphragm in a single process, from the same material by means<br />

<strong>of</strong> plastic injection mol<strong>din</strong>g. This is possible by the progress in the field <strong>of</strong> this<br />

mol<strong>din</strong>g process, where pressure diaphragms as thin as 75 µm are possible to be<br />

obtained. As plastic materials one can mention here, polycarbonates, polyesters<br />

such as PET or nylon, or PVC.<br />

As mentioned from very beginning, one <strong>of</strong> the most important drivers for such allplastic<br />

piezoresistive pressure sensors, based on injection mol<strong>din</strong>g and direct<br />

printing <strong>of</strong> the organic conductive and piezoresistive solid films is the high<br />

potential for a low cost fabrication process and associated materials. Such<br />

concepts show the potential <strong>of</strong> the organic semiconductors to open the way<br />

towards a new family <strong>of</strong> applications like flexible, intelligent microsystems,<br />

where both the electronic circuit signal processing and the sensing <strong>de</strong>vices to be<br />

performed on the organic substrate.<br />

5. Conclusions<br />

In this paper we have reviewed the key materials and processes for the realization<br />

<strong>of</strong> the polymeric thick films piezoresistive, and we introduced our concepts for the<br />

preparation <strong>of</strong> novel organic piezoresistive thin films to be used in the next<br />

generation <strong>of</strong> piezoresistive pressure sensor on rigid and flexible substrates.<br />

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Polymeric Pressure Sensors:<br />

A Conceptual View 81<br />

The polymeric pressure sensor domain was <strong>de</strong>veloped in the last two <strong>de</strong>ca<strong>de</strong>s<br />

starting from the useful results obtained in the years 1980‟s on piezoresistive<br />

ruthenate thick films. Such polymeric thick films consisted <strong>of</strong> carbon loa<strong>de</strong>d<br />

polyimi<strong>de</strong> films have shown a gauge factor <strong>of</strong> about 10, and they have been used<br />

for pressure sensor operating in the range <strong>of</strong> about 0-10 6 Pa on either rigid or<br />

flexible substrate.<br />

The relatively high temperature coefficient <strong>of</strong> resistance (+/- 500 ppm/ o C) and<br />

long-term drift <strong>of</strong> these organic polymeric piezoresistive films (0.5-2)% used for<br />

either planar and sandwich <strong>de</strong>vice configuration are partially solved by<br />

Wheatstone bridge-based signal conditioning.<br />

More work should be further <strong>de</strong>voted to the repeatability <strong>of</strong> fabrication<br />

technology so that the organic piezoresistors connected in the Wheatstone bridge<br />

to have similar temperature coefficient <strong>of</strong> resistance and gauge factor, and thus<br />

minimize the long- term drift <strong>of</strong> sensor output.<br />

We have introduced two novel approaches for the preparation <strong>of</strong> the thin film<br />

polymeric piezoresistive pressure sensors. First concept consisted in the selective<br />

surface modification <strong>of</strong> the organic substrate by ion implantation <strong>of</strong> nitrogen<br />

species for inducing local piezorestivity, followed by phosphorus or boron<br />

implantion for enhancing the electrical conductivity or the organic piezoresistors.<br />

The novelty <strong>of</strong> the second concept consisted in the original chemical synthesis <strong>of</strong><br />

piezoresistive organic material, <strong>de</strong>position method by direct printing, and<br />

monolithic fabrication <strong>of</strong> plastic diaphragm by injection mol<strong>din</strong>g.<br />

The new organic synthesis consist in doping <strong>of</strong> polyaniline as free base(<br />

emeral<strong>din</strong>e) with large organic molecules (p-sulfonated calix[n]arenes p-<br />

sulfonated calix[n]arenes, tosylates, carboxylic acids <strong>of</strong> calix[n]arenes, sulfonated<br />

crown ethers, sulfonated cyclo<strong>de</strong>xtrines, carboxylic acid nanotubes, or carboxylic<br />

acid <strong>of</strong> fullerenes. The bulk counterions <strong>of</strong> dopants improve the conductivity <strong>of</strong><br />

polyanilines<br />

Acknowledgement<br />

The authors would like to expresses their thanks to Honeywell International for<br />

their support to work on this topic and write this paper.<br />

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82 Cornel Cobianu, Bogdan Serban<br />

R E F E R E N C E S<br />

[1] Ch.Smith, “Piezoresistive effect in germanium and silicon”, Physical Review, 1954, vol. 94,<br />

pp. 42-49.<br />

[2] Commercial <strong>de</strong>vices have been available for some time. See, for example, the “National<br />

Semiconductor Catalog”, Transducers; Pressure and Temperature for August 1974.<br />

[3] G. Harsanyi, “Polymer Thick Films Technology: a Possibility to Obtain Very Low Cost<br />

Pressure Sensors?”, Sensors and Actuators A, 25-25 (1991), pp. 853-857.<br />

[4] C. Csazar, G.r Harsanyi and R. P. Agarwal, “A very low cost pressure sensor with extremely<br />

high sensitivity”, Sensors and Actuators A, vol. 41-42 (1994), pp. 417-420.<br />

[5] K.I. Arshak, A.K. Ray, C.A. Hogarth, D.G.Collins, F. Ansari, “An Analysis <strong>of</strong> polymeric thick<br />

films as pressure sensors”, Sensors and Actuators, A 4 vol. 49, (1995) pp. 41-45.<br />

[6] N.J. Hendreson, N.M. White, T.V. Papakostas, P.H. Hartel, “Low-Cost planar PTF Sensors<br />

for I<strong>de</strong>ntity Verification <strong>of</strong> Smartcard Hol<strong>de</strong>rs” , Invited paper 2002 IEEE, “Flexible Sensors in<br />

Smart Applications” session.<br />

[7] C. Cobianu, M. Gologanu, I. Pavelescu, B. Serban, “Micro-machined Pressure Sensor with<br />

Polymer Diaphragm”, US Patent 7401525 B2, Date <strong>of</strong> Patent July 22, 2008.<br />

[8] C. Cobianu, S. R. Shiffer, B. Serban, A.D. Bradley, M. N. Mihaila, “Pressure Sensor”,<br />

US Patent 7 318351 B2, Date <strong>of</strong> Patent, January 15, 2008.<br />

[9] C. Canali, D. Malavasi, B. Moretn, M. Pru<strong>de</strong>nziati, A. Taroni, “Strain Sensitivity in Thick Film<br />

Resistors”, IEEE Transactions on Components, Hybrids, and Manufacturing Technology, vol.<br />

CHMT-3, No. 3, September 1980, pp. 421-423.<br />

[10] R. P. Arreny and J. G. Webster, “Sensors and Signal Conditioning”, Second Edition, John<br />

Wiley and Sons, 2001, ISBN 0-471-33232-1.<br />

[11] D. Shavit: “The <strong>de</strong>velopments <strong>of</strong> LEDs and SMD Electronics on Transparent Conductive<br />

Polyester Film”, Vacuum International, 1/2007, S. 35 ff.<br />

[12] H. Sirringhaus, C.W. Sele, T. von Werne, C. Ramsdale, 2007 “Manufacturing <strong>of</strong> organic<br />

Transistor Circuits by Solution-based Printing” in G. Hadziioannou, G.G. Malliaras,<br />

“Semiconducting Polymers: Chemistry, Physics and Engineering”, vol. 2 (2 nd Edition),Wiley-<br />

VCH. pp. 667–694. ISBN 978352731271913]<br />

[13] R. E. Giedd, M.G. Moss, M.M. Craig, and D.E. Robertson, “Temperature sensitive ionimplanted<br />

polymer films," Nuclear Instruments and Methods in Physics Research [Netherlands],<br />

vol. B59/60, 1991, pp. 1253-1256.<br />

[14] B. Serban, M. Bercu, S. Voicu, M. Mihailă, Gh. Nechifor, C. Cobianu “Calixarene –doped<br />

polyaniline for applications in sensing”, International Semiconductor Conference, CAS 2006,<br />

Procee<strong>din</strong>gs, pp. 257-260.<br />

[15] M. Hedges, “Aerosol Jet Technology for Printed and Organic Electronic Devices”,<br />

Procee<strong>din</strong>gs <strong>of</strong> LOPE Conference, 2009.<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066-8562 Volume 5, Number 1/2012 83<br />

AN ANALYSIS REGARDING THE DECREASING OF THE<br />

IMAGE QUALITY WITH THE OPTICAL MISALIGNMENT<br />

CATALIN SPULBER 1 , OCTAVIA BORCAN 2<br />

Rezumat. Performantele <strong>de</strong> informație vizuala achiziționate <strong>de</strong> o camera termala sunt<br />

<strong>de</strong>terminate <strong>de</strong> doi parametri distincți, NETD (Noise equivalent temperature difference)<br />

si MTF (Modulation Transfer Function); valoarea fiecăruia <strong>din</strong>tre acești parametri este<br />

<strong>de</strong>pen<strong>de</strong>ntă <strong>de</strong> caracteristicile si <strong>de</strong> metodologia <strong>de</strong> măsurare a componentelor <strong>de</strong> bază<br />

ale unei camere termale: obiectivul și matricea <strong>de</strong> <strong>de</strong>tecție. Autorii analizează unele<br />

probleme legate <strong>de</strong> măsurarea NETD și a MTF în cazul în care variază distanța focală a<br />

obiectivului și apare o <strong>de</strong>zaliniere optică la montajul camerei termale. Experimentele<br />

realizate <strong>de</strong>monstrează că o distanță focală mai mare asigură un MTF mai bun, iar<br />

evaluarea NETD cu instrumentar electronic este mai a<strong>de</strong>cvată.<br />

Abstract. The performances <strong>of</strong> visual information acquired with a thermal camera are<br />

<strong>de</strong>termined by two distinct parameters, NETD (Noise equivalent temperature difference)<br />

and MTF (Modulation Transfer Function) values <strong>of</strong> each <strong>of</strong> these parameters is<br />

<strong>de</strong>pen<strong>de</strong>nt on the characteristics and the methodology for measuring the basic<br />

components <strong>of</strong> thermal camera: the lens and the starring <strong>de</strong>tector. The authors analyze<br />

some problems related to measurement NETD and MTF where the focal lens is variable<br />

and optical misalignment occurs when mounting thermal camera. Experiments<br />

<strong>de</strong>monstrate that a longer focal distance provi<strong>de</strong>s a better MTF and NETD evaluation<br />

with electronic instruments is most appropriate.<br />

Keywords: Thermal camera, NETD, MTF, optical misalignment, lens focal<br />

1. Introduction<br />

It is known that, in the field <strong>of</strong> actual research <strong>of</strong> vision using thermal cameras,<br />

the most frequent question refers to the performance <strong>of</strong> the distance observation,<br />

as is shown in the paper [1, 2].<br />

This performance is <strong>de</strong>scribed by some main parameters, as Noise Equivalent<br />

Temperature Difference (NETD), Modulation Transfer Function (MTF), and<br />

Minimum Resolvable Temperature Difference (MRTD) [3].A thermal camera is<br />

commonly composed <strong>of</strong> an optical assembly, a FPA <strong>de</strong>tector module (starring<br />

<strong>de</strong>tector), and signal processing electronics.<br />

The imaging process can be <strong>de</strong>scribed as a functional flow diagram (fig. 1.) from<br />

scene (input information) to observer (output information).<br />

1 Pro Optica Service&Components, e-mail: catalin.spulber@yahoo.com., Aca<strong>de</strong>my <strong>of</strong> Romanian<br />

Scientists, www.aosromania.ro.<br />

2 Pro Optica Service&Components, Romania, e-mail: borcan_octavia@yahoo.com.<br />

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84 Catalin Spulber, Octavia Borcan<br />

Fig. 1. The flow information between thermal camera components.<br />

The lens gathers the scene radiance onto the <strong>de</strong>tector array (FPA). The <strong>de</strong>tector<br />

module converts the radiation (photons) into an electrical signal, which enters a signal<br />

processing unit. As it already was mentioned by authors in a previous article [2], the<br />

environment (the atmosphere with aerosols or thermal perturbations) and the main<br />

components <strong>of</strong> camera can <strong>de</strong>teriorates the final image.<br />

An object is visible in an image because it has a different brightness than its<br />

surroun<strong>din</strong>gs (target contrast). The input to any thermal camera system is photon<br />

number N from the scene. The contrast <strong>of</strong> the object (i.e., the signal) must overcome<br />

the image noise. Noise increases with the signal level results when the image has<br />

been represented by a small number <strong>of</strong> individual particles. The signal-noise ratio<br />

(SNR) is <strong>de</strong>fined as the contrast divi<strong>de</strong>d by the standard <strong>de</strong>viation <strong>of</strong> the noise [4].<br />

The mathematics governing these variations is called counting statistics or Poisson<br />

statistics. That is, if there are N particles in each pixel on display, the mean is equal to<br />

N and the standard <strong>de</strong>viation is equal to N . This makes the signal-to-noise ratio<br />

equal to N . Detection is a noisy process. The noise V is composed <strong>of</strong> shot noise,<br />

spatial noise, and excess noise. There are additional noise sources, inclu<strong>din</strong>g readout<br />

amplifier noise and digital quantization noise. This is mo<strong>de</strong>lled as follows [4]:<br />

V V read V noise<br />

(1)<br />

The noise equivalent temperature difference (NETD) is a wi<strong>de</strong>ly used performance<br />

parameter that characterizes the sensitivity <strong>of</strong> thermal imaging sensors.<br />

The Modulation Transfer Function (MTF) is a quantitative measure <strong>of</strong> thermal<br />

camera capability to transfer contrasts from the object plan in the image plan<br />

<strong>de</strong>pen<strong>din</strong>g on the aims <strong>of</strong> the lens and <strong>de</strong>tector <strong>de</strong>tails. MTF is used to approximate<br />

the position <strong>of</strong> best focus.<br />

2. The problematic<br />

Two problems are import ants if there is misalignment between the optical lens<br />

and FPA:<br />

a) Although NETD has been used for many years, there has always been some<br />

confusion and misun<strong>de</strong>rstan<strong>din</strong>g about how to measure it. Differences in opinion<br />

on how this measurement should be ma<strong>de</strong> can cause substantial variations in<br />

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An Analysis Regar<strong>din</strong>g the Decreasing <strong>of</strong> the Image Quality<br />

with the Optical Misalignment<br />

reported values <strong>of</strong> NETD measurements [5]; for example, subjective digital noise<br />

introduced by the display. The NETD will then calculated from the experimental<br />

data as follows [6,7]:<br />

NETD T<br />

(2)<br />

S/ N<br />

T T t T<br />

where arg et<br />

thermal camera.<br />

background , and the SNR is the signal-to-noise ratio <strong>of</strong> the<br />

b) The projection <strong>of</strong> the scene on the FPA <strong>de</strong>tector is not perfect; since the<br />

optical elements create blur [8]. For a quantitative analysis it used a test thermal<br />

pattern as in figure 2., and the relation [3]:<br />

MTF<br />

MTFoptics<br />

MTFFPA<br />

MTFdisplay<br />

MTFeye<br />

(3)<br />

Fig. 2. Thermal pattern used in the thermal camera performance analysis.<br />

The MTF value varies with the lens focal length and their aperture or F number<br />

(F#). The calculus <strong>of</strong> MTF values is based on the followings relations:<br />

MTFFPA<br />

<br />

f<br />

<br />

sin<br />

<br />

<br />

fcut<strong>of</strong>f<br />

<br />

f<br />

<br />

<br />

<br />

fcut<strong>of</strong>f<br />

<br />

f<br />

sinc<br />

<br />

fcut<strong>of</strong>f<br />

where the spatial frequency f [cycles/mm], the cut-<strong>of</strong>f frequency c ut-<strong>of</strong>f [cycles/mm],<br />

the horizontal and vertical size <strong>of</strong> <strong>de</strong>tector (dH and dV, respectively) is exprimed as:<br />

1 lp<br />

1 lp<br />

fcut<strong>of</strong>f<br />

H [ ];fcut<strong>of</strong>f<br />

V [ ];<br />

<br />

dasH mrad<br />

dasV mrad<br />

dH<br />

dV<br />

dasH [mrad];dasV [mrad]<br />

fob<br />

fob<br />

<br />

<br />

<br />

(4)<br />

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86 Catalin Spulber, Octavia Borcan<br />

d <br />

<br />

CCH<br />

MTF display (fH<br />

) sinc FFH<br />

fH<br />

(5) where FF H and FF V –fill factors for<br />

fl <br />

<strong>de</strong>tector on the horizontal, respectively vertical direction.<br />

MTF optics and MTF FPA have the configuration in figure 3.<br />

where<br />

Fig. 3. MTF Diagram for the MTF realized with the Maviis 1.5 s<strong>of</strong>tware (JCD Publishing).<br />

On the other hand, it is known that [3, 9]:<br />

( V1<br />

V4<br />

)<br />

MTF <br />

(6)<br />

( V V<br />

) 4<br />

1<br />

MTF(t t<br />

4<br />

<br />

NETD <br />

1/ 2<br />

3 f <br />

1/ 2 <br />

T<br />

( f<br />

<br />

R ) d <br />

MRTD <br />

(7)<br />

<br />

<br />

frame<br />

1/ 2<br />

1/ 2<br />

)<br />

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An Analysis Regar<strong>din</strong>g the Decreasing <strong>of</strong> the Image Quality<br />

with the Optical Misalignment<br />

or [7]:<br />

MRTD<br />

f<br />

K NETD<br />

f<br />

(8)<br />

MTF<br />

f<br />

where: f R -electronic frequency bandwidth, - the field <strong>of</strong> view <strong>of</strong> the FPA<br />

starring, f-the spatial frequency <strong>of</strong> the target being observed, d [s]– response time<br />

<strong>of</strong> the <strong>de</strong>tector, t- the integration time <strong>of</strong> the observer eye, t frame - the frame time.<br />

So, it can write:<br />

NETD <br />

MTF(f ) const1<br />

<br />

;<br />

MRTD(f )<br />

const<br />

NETD 2<br />

;<br />

<br />

1<br />

<br />

(9)<br />

f f<br />

For comparison <strong>of</strong> two MRTD as the same spatial frequency, in which one <strong>of</strong> the<br />

thermal camera has a certain optical misalignment, it can by written as:<br />

3. Experiments and results<br />

ob <br />

MRTD(f ) MTFmis<br />

(f ) NETD<br />

<br />

(10)<br />

MRTDmis<br />

(f ) MTF(f ) NETDmis<br />

For the experimental <strong>de</strong>termination a thermal camera with the following technical<br />

characteristics was used: the working spectral range 812 μm, <strong>de</strong>tection matrix<br />

with micro-bolometers and resolution <strong>of</strong> 640 x 480 <strong>de</strong>tection items, the size <strong>of</strong> the<br />

<strong>de</strong>tection item being 0.17 μm, the focal distance for the objective being <strong>of</strong> 45 and<br />

135 mm and f number (F#) between f/1.1 (for 45 mm lens focal) and f/1.6 (for<br />

135 mm lens focal). In laboratory conditions, in or<strong>de</strong>r to <strong>de</strong>termine the MRTD<br />

function thermal patterns with 4 cycles/target, the ambient temperature was<br />

24.7 0 C, and the black body temperature was 29.7 0 C (fig.4-6).<br />

Fig. 4. Example <strong>of</strong> image<br />

acquired with thermal contrast<br />

T = 10 C<br />

Fig. 5. Example <strong>of</strong> image<br />

acquired with thermal contrast<br />

T=5 C<br />

Fig. 6. Example <strong>of</strong> image<br />

acquired with thermal contrast<br />

T=2 C<br />

The procedure used to evaluate NETD was based on standard ASTM E 1543-00 [6].<br />

The results are presented in figures 7-19.<br />

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Signal, Noise, NETD [mV]<br />

88 Catalin Spulber, Octavia Borcan<br />

Fig. 7. Visual images signal and noise on the oscilloscope.<br />

140<br />

Signal S [mV]<br />

120<br />

100<br />

80<br />

60<br />

40<br />

20<br />

NETD<br />

Noise N [mV]<br />

0<br />

0 1 2 3 4 5 6 7 8 9<br />

Measurement no.<br />

Fig. 8. Variation <strong>of</strong> the NETD exclu<strong>din</strong>g subjective (digital) noise.<br />

Fig. 9. Original Image for measurement MTF (aligned focal lens 135 mm) with DT 1500<br />

tester thermal camera and related s<strong>of</strong>tware from Inframet.<br />

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An Analysis Regar<strong>din</strong>g the Decreasing <strong>of</strong> the Image Quality<br />

with the Optical Misalignment<br />

Fig. 10. The diagram MTF vs. spatial frequency. The loss <strong>of</strong> image quality in different cases <strong>of</strong> a<br />

lens misalignment with 45 mm focal length.<br />

Fig. 11. The diagram contrast vs. <strong>of</strong>f-axis distance.<br />

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90 Catalin Spulber, Octavia Borcan<br />

The loss <strong>of</strong> image contrast with <strong>of</strong>f-axis distance <strong>of</strong> a 45 mm focal length.<br />

Fig. 12. The diagram MTF vs. spatial frequency. Comparison between MTF diagrams for lenses<br />

with 45 mm and 135 mm focal lengths, with well alignment done. One can see, for example, that<br />

for a same resolution <strong>of</strong> 0,5 lp/mm, a 3.3 times improvement <strong>of</strong> contrast using a lens with a focal<br />

length 3 times greater, can be obtained.<br />

Fig. 13. MTF aligned focal lens 45 mm.<br />

Fig. 14. MTF aligned focal lens 135 mm.<br />

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An Analysis Regar<strong>din</strong>g the Decreasing <strong>of</strong> the Image Quality<br />

with the Optical Misalignment<br />

Fig. 15. MTF with misaligned<br />

2 mm focal lens 135 mm.<br />

Fig. 16. MTF with misaligned<br />

2 mm focal lens 45 mm.<br />

Fig. 18. MTF with misaligned<br />

5 mm focal lens 135 mm.<br />

Fig. 19. MTF with misaligned<br />

5 mm focal lens 45 mm.<br />

4. Conclusions<br />

A better MTF and NETD evaluation with electronic instruments is most<br />

appropriate;<br />

A significant <strong>de</strong>crease in MTF is obtained at low level variations <strong>of</strong> optical<br />

misalignement;<br />

4.3 The MTF <strong>de</strong>creases with <strong>de</strong>creasing lens focal.<br />

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92 Catalin Spulber, Octavia Borcan<br />

R E F E R E N C E S<br />

[1] Owen, A.: "Surveillance cameras steal away the night”, in Laser Focus World, 33, 111-115 (1997).<br />

[2] Borcan, Octavia, Spulber, C: ”Experimental method for observation prediction based on the<br />

<strong>de</strong>cision matrix, through day/night equipments in NIR and LWIR spectral ranges, in Infrared Imaging<br />

Systems: Design, Analysis, Mo<strong>de</strong>lling, and Testing XX, edited by Gerald C. Holst, Procee<strong>din</strong>gs <strong>of</strong><br />

SPIE Vol. 7300 (SPIE, Bellingham, WA 2009) 730011.<br />

[3] Holst, Gerald C. Infrared Imaging Systems: Design, Analysis, Mo<strong>de</strong>lling, and Testing IX.<br />

[4] Saar Bobrov* and Yoav Y. Schechner: ”Image-based prediction <strong>of</strong> imaging and vision<br />

performance”, in J. Opt. Soc. Am. A/Vol. 24, No. 7/July 2007.<br />

[5] Ronald G. Driggers, Curtis M. Webb, Stanley J. Pruchnic, Carl E. Halford and Ellis E. Burroughs,<br />

"Laboratory measurement <strong>of</strong> sampled infrared imaging system performance", in Opt. Eng. 38, 852<br />

(1999).<br />

[6] ***ASTM E 1543 – 00: Standard Test Method for Noise Equivalent Temperature Difference <strong>of</strong><br />

Thermal Imaging Systems.<br />

[7] Arnold Daniels: ”Field Gui<strong>de</strong> to Infrared Systems Field Gui<strong>de</strong> to Infrared Systems, Detectors, and<br />

FPAs, Second Edition”, SPIE Press Book, Bellingham, 2010, ISBN: 9780819480804.<br />

[8] Steven W.Smith: The Scientist and Engineer's Gui<strong>de</strong> to Digital Signal Processing, 1997, ISBN<br />

978-0966017632.<br />

[9] Alan Irwin, Robert L. Nicklin:”Standard s<strong>of</strong>tware for automated testing <strong>of</strong> infrared imagers,<br />

IRWindows, in practical applications”, in Procee<strong>din</strong>gs <strong>of</strong> SPIE, SPIE 3377, 206 (1998).<br />

[10] Paul A. Bell, Carl W. Hoover, Jr., Stanley J. Pruchnic, Jr., “Standard NETD test procedure for<br />

FLIR systems with vi<strong>de</strong>o outputs”, Proc. SPIE 1969, 194 (1993].<br />

[11] Spulber, C, Borcan, Octavia: “Some Aspects Regar<strong>din</strong>g the Image Acquisition using Vi<strong>de</strong>o<br />

Systems un<strong>de</strong>r Low Vibrations”, in Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists Series on Science<br />

and Technology <strong>of</strong> Information 6, Vol. 2, 87-98, Number 1/2009, ISSN 2066–2742.<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066-8562 Volume 5, Number 1/2012 93<br />

APPLICATIONS OF QUANTUM CRYPTOLOGY<br />

FOR DATA TRANSMISSIONS<br />

IMPLEMENTED IN A STUDENT LABORATORY<br />

Bogdan-Adrian STEFANESCU 1 , Dan ANGHEL 1 , Octavian DANILA 1 ,<br />

Paul STERIAN 1 , Andreea Rodica STERIAN 1<br />

Abstract. Quantum cryptography based on the BB84 protocol is discussed in the<br />

following presentation, containing the concepts and the work that has been carried out in<br />

the field, with some <strong>de</strong>velopments suitable for stu<strong>de</strong>nt research. Although it has not been<br />

implemented on a commercial level, data transmissions based on quantum cryptology is a<br />

good alternative for integration in optical fibers communications, with a wi<strong>de</strong> range <strong>of</strong><br />

applications due to its’ securing capabilities. Evolution in photon-study related fields,<br />

such as photon echo, contribute to the better un<strong>de</strong>rstan<strong>din</strong>g and further improvement <strong>of</strong><br />

the quantum key distribution protocol. An efficient way <strong>of</strong> encrypting the information is<br />

by the use <strong>of</strong> a key. As it is well known, the encryption key uses very complex algorithms<br />

that are very hard to break but the problem <strong>of</strong> key transmission between the transmitter<br />

and receiver still remains. On a classical channel, the answer was given in the form <strong>of</strong><br />

RSA public keys that were sent between the transmitter and receiver several times, and<br />

implied the use <strong>of</strong> randomizing algorithms by use <strong>of</strong> prime numbers. Quantum approach<br />

<strong>of</strong> this problem can be solved through the following principle: If a quantum system that<br />

resi<strong>de</strong>s in a <strong>de</strong>fined state is observed, thus measured, the state <strong>of</strong> that system is<br />

irreparably changed. This has a direct application in <strong>de</strong>tecting whether an eavesdropper<br />

has entered the quantum channel or not. A stu<strong>de</strong>nt-oriented experimental apparatus is<br />

presented, together with a virtual simulation <strong>of</strong> the protocol that implements the<br />

principles <strong>of</strong> quantum cryptography. Our optical channel can be improved using the<br />

photon echo effect. Excitement <strong>of</strong> superradiant states by irradiating a probe with a<br />

coherent optical impulse, with its duration and intensity conveniently chosen can be<br />

shown with the photon echo. We <strong>de</strong>monstrated that the photon echo can improve the co<strong>de</strong><br />

by ad<strong>din</strong>g either a controlled error on the channel or transforming the channel from a<br />

binary channel to a ternary channel.<br />

Keywords: Quantum cryptology, Data transmission, superradiant states, ternary channel<br />

1. Introduction<br />

The goal <strong>of</strong> this paper is to help stu<strong>de</strong>nts un<strong>de</strong>rstand the application <strong>of</strong> quantum<br />

physics in information security.<br />

Why is information security so important? In present days, a lot <strong>of</strong> information is<br />

exchanged via large networks, such as a LAN or the Internet [1-3, 11]. If sensitive<br />

information is exchanged, a way <strong>of</strong> guar<strong>din</strong>g the information from unwanted<br />

eavesdroppers is nee<strong>de</strong>d [4-6]. A quite simple way <strong>of</strong> doing this is by encrypting<br />

1 Aca<strong>de</strong>mic Center for Optical Engineering and Photonics, Faculty <strong>of</strong> Applied Sciences, University<br />

“Politehnica” Bucharest, Romania (sterian@physics.pub.ro).<br />

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the information. An efficient way <strong>of</strong> encrypting the information is by the use <strong>of</strong> a<br />

key. The encryption key uses very complex algorithms that are very hard to break,<br />

but there is another problem: How does the sen<strong>de</strong>r send the key to the receiver? In<br />

early days, the key was transported to the receiver via physical medium such as<br />

paper, punch card, floppy disk, EEPROM or CDROM. There was no insurance <strong>of</strong><br />

the interception <strong>of</strong> the key.<br />

On a classical channel, used in the 1970-s, the answer was given in the form <strong>of</strong><br />

RSA public keys[5], that were sent between the transmitter and receiver several<br />

times, and implied the use <strong>of</strong> randomizing algorithms by use <strong>of</strong> prime numbers.<br />

Quantum approach <strong>of</strong> this problem can be solved through the following principle:<br />

If a quantum system that resi<strong>de</strong>s in a <strong>de</strong>fined state is observed, thus measured, the<br />

state <strong>of</strong> that system is irreparably changed. This has a direct application in<br />

<strong>de</strong>tecting whether or not an eavesdropper has entered the quantum channel.<br />

2. Quantum Cryptography<br />

Quantum cryptography solves the key distribution problem by allowing the<br />

exchange <strong>of</strong> a cryptographic key between two remote parties with absolute<br />

security, guaranteed by the laws <strong>of</strong> physics. This key can then be used with<br />

conventional cryptographic algorithms [5]. If one enco<strong>de</strong>s the value <strong>of</strong> a digital bit<br />

on a single quantum object, its interception will necessarily translate into a<br />

perturbation, because the eavesdropper is forced to observe it. This perturbation<br />

causes errors in the sequence <strong>of</strong> bits exchanged by the sen<strong>de</strong>r and recipient. By<br />

checking for the presence <strong>of</strong> such errors, the two parties can verify whether their<br />

key was intercepted or not. It is important to stress that since this verification<br />

takes place after the exchange <strong>of</strong> bits, one finds out a posteriori whether the<br />

communication was eavesdropped or not. That is why this technology is used to<br />

exchange a key and not valuable information. Once the key is validated, it can be<br />

used to encrypt data. In telecommunication networks, light is routinely used to<br />

exchange information. For each bit <strong>of</strong> information, a pulse is emitted and sent<br />

down an optical fiber to the receiver, where it is registered and transformed back<br />

into an electronic signal. These pulses typically contain millions <strong>of</strong> photons [3,<br />

14]. In quantum cryptography, one can follow the same approach, with the only<br />

difference that the pulses contain only a single photon. In particular a photon<br />

cannot be split into halves.[6].<br />

3. The BB84 protocol<br />

The first protocol for QC has been proposed in 1984 by Charles H. Bennett, from<br />

IBM New-York, and Gilles Brassard, from the University <strong>of</strong> Montreal, hence the<br />

name BB84 un<strong>de</strong>r which this protocol is recognized nowadays. They published<br />

their work in a conference in India, totally unknown to physicists.<br />

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We shall explain the BB84 protocol using the language <strong>of</strong> spin 1/2 , any 2 level<br />

system being equivalent to it. The protocol uses two interlocutors, Alice, as the<br />

transmitter, and Bob, the receiver, as well as an eavesdropper, Eve. The photons<br />

<strong>of</strong> use are divi<strong>de</strong>d into 4 quantum states that constitute 2 bases, think <strong>of</strong> the states<br />

up | ↑i, down | ↓i, left | ←i and right | →i. Conventionally, one attributes the<br />

binary value 0 to states | ↑i and | →i and the value 1 to the other two states, and<br />

calls the states qubits (for quantum bits). In the first step, Alice sends individual<br />

spins to Bob in states chosen at random among the 4 basic states (the spin states |<br />

↑i,| ↓i, | →i and | ←i are i<strong>de</strong>ntified with the polarization states ”horizontal”,<br />

”vertical”, ”+45 <strong>de</strong>grees” and ”-45 <strong>de</strong>grees”, respectively). How she ”chooses at<br />

random” is a <strong>de</strong>licate problem in practice, but in principle she could use her free<br />

will. The individual spins could be sent all at once, or one after the other (much<br />

more practical); the only restriction being that Alice and Bob can establish a oneto-one<br />

correspon<strong>de</strong>nce between the transmitted and the received spins[1]. Next,<br />

Bob measures the incoming spins in one <strong>of</strong> the two bases, chosen at random<br />

(using a random number generator in<strong>de</strong>pen<strong>de</strong>nt from that <strong>of</strong> Alice). At this point,<br />

whenever they used the same basis, they get perfectly correlated results. However,<br />

whenever they used different basis, they get uncorrelated results. Hence, on<br />

average, Bob obtains a string <strong>of</strong> bits with 25% errors, called the raw key. This<br />

error rate is so large that standard error correction schemes would fail. But in this<br />

protocol Alice and Bob know which bits are perfectly correlated (the ones for<br />

which Alice and Bob used the same basis) and which ones are completely<br />

uncorrelated (all the other ones). Hence, a straightforward error correction scheme<br />

is possible: For each bit Bob announces publicly in which basis he measured the<br />

correspon<strong>din</strong>g qubit (but he does not tell the result he obtained). Alice then only<br />

tells whether or not the state in which she enco<strong>de</strong>d that qubit is compatible with<br />

the basis announced by Bob. If the state is compatible, they keep the bit, if not<br />

they disregard it. In this way about 50% <strong>of</strong> the bit string is discar<strong>de</strong>d. This shorter<br />

key obtained after bases reconciliation is called the sifted key. The fact that Alice<br />

and Bob use a public channel at some stage <strong>of</strong> their protocol is very common in<br />

crypto-protocols. This channel does not have to be confi<strong>de</strong>ntial, but has to be<br />

authentic. Hence, any adversary Eve can listen to it all the communication on the<br />

public channel, but she can’t modify it. In practice Alice and Bob may use the same<br />

optical fiber to implement both the quantum and the classical channels. Note that<br />

neither Alice nor Bob can <strong>de</strong>ci<strong>de</strong> which key results from the protocol. In<strong>de</strong>ed, it is<br />

the conjunction <strong>of</strong> both <strong>of</strong> their random choices which produces the key [4-6].<br />

Let us now consi<strong>de</strong>r the security <strong>of</strong> the above i<strong>de</strong>al protocol (i<strong>de</strong>al because so far<br />

we did not take into account unavoidable noise due to technical imperfections).<br />

Assume that some adversary Eve intercepts a qubit propagating from Alice to<br />

Bob. This is very easy, but if Bob does not receive an expected qubit, he will<br />

simply inform Alice to disregard it. Hence, in this way Eve only lowers the bit<br />

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rate (possibly down to zero), but she does not gain any useful information. For<br />

real eavesdropping Eve must send a qubit to Bob. I<strong>de</strong>ally she would like to send<br />

this qubit in its original state, keeping a copy for herself.<br />

4. Simple s<strong>of</strong>tware simulation <strong>of</strong> the BB84 protocol<br />

There are many s<strong>of</strong>tware implementations used to simulate the BB84 protocol.<br />

Some are written in PHP co<strong>de</strong>, Java ,C++, or native quantum simulation s<strong>of</strong>tware.<br />

For this paper we have chosen a s<strong>of</strong>tware written in Visual C++ called QIT<br />

<strong>de</strong>signed by Fernando Lucas Rodriguez. This is a general public license (GPL)<br />

s<strong>of</strong>tware and it can be found on the Internet for stu<strong>de</strong>nt training and research. The<br />

program has an interactive graphical user interface (GUI) that allows stu<strong>de</strong>nts to<br />

watch a step by step execution <strong>of</strong> the protocol. Stu<strong>de</strong>nts will use the program to<br />

find the different quantum keys.<br />

The program will run from one <strong>of</strong> the 2 computers on the lab table witch must run<br />

a Windows XP 2 operating system with .NET 2 installed. From the fol<strong>de</strong>r QIT13<br />

the stu<strong>de</strong>nts must execute QIT IDE.exe [9]. After the execution the following<br />

window will appear (Fig. 1.):<br />

Fig. 1. Output window <strong>of</strong> QIT.exe<br />

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Applications <strong>of</strong> Quantum Cryptology for Data Transmissions<br />

Implemented in a Stu<strong>de</strong>nt Laboratory 97<br />

Then from the Interactive menu ->Communications->InteractiveBB84<br />

Cryptosystem is selected. With this selection the interface for simulating the<br />

BB84 protocol will appear (Fig. 2.):<br />

Fig.2. GUI <strong>of</strong> QIT.exe<br />

Example: The secret data to be sent is: “Information Security and Cryptology”.<br />

Press Start, then Finish. The resulting binary secret key is:<br />

110101001101110011010000101010000000010011110111101101111001000010<br />

011000110101011110101111010000010101001001010011100100110111100000<br />

000010010001100111101110110101011010001010111010100110010101110010<br />

010110000000001011000101101011100010111110001010000111000000111110<br />

1100100111000100<br />

A step by step execution <strong>of</strong> the protocol is available by pressing Start then<br />

Execute Step [9].<br />

The figure 1 and 2 represent the main steps in the execution <strong>of</strong> the protocol.<br />

Behind the s<strong>of</strong>tware the steps are as follow: the (4+<strong>de</strong>lta)·N qubits will be<br />

transmitted. For each bit, Master station selects a basis randomly (horizontalvertical<br />

or diagonal), and also selects a random value (true or false). It sends the<br />

resulting quantum state after enco<strong>din</strong>g the true or false value into the selected basis.<br />

It also stores the basis selected and the random value. The slave station measures<br />

values received into a random basis (horizontal-vertical or diagonal). It stores the<br />

basis used for measurement and the value measured. The master station sends the<br />

basis used for values enco<strong>din</strong>g. The values are not transmitted, they are the secret.<br />

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The slave station stores the master's used basis for enco<strong>din</strong>g. The master station<br />

stores coinci<strong>de</strong>nces. Slave station informs Master about which basis there was<br />

coinci<strong>de</strong>nce during qubit enco<strong>din</strong>g and slave measurement. Values measured are<br />

not transmitted, only if there was coinci<strong>de</strong>nce.<br />

The master and slave generates an intermediary 'secret private' key with the values <strong>of</strong><br />

qubits <strong>of</strong> which where was coinci<strong>de</strong>nce on basis enco<strong>din</strong>g and measurement and<br />

checks that intermediary key has at least the double <strong>of</strong> bits nee<strong>de</strong>d for chippering data.<br />

The master select random intermediary-key bits in<strong>de</strong>xes for public comparisons,<br />

and informs <strong>of</strong> those positions to the slave. The number <strong>of</strong> bits to compare will be<br />

the size <strong>of</strong> intermediary key minus the number <strong>of</strong> bits nee<strong>de</strong>d for chippering data.<br />

Slave stores the in<strong>de</strong>xes <strong>of</strong> the positions that will be compared.<br />

The master sends the values that tried to enco<strong>de</strong> on quantum channel <strong>of</strong> the selected<br />

in<strong>de</strong>xes. Slave stores the values that Master sends. The master stores the values that<br />

Slave sends. Slave sends the values that measured on quantum channel <strong>of</strong> the<br />

selected in<strong>de</strong>xes.<br />

Master calculates noise level (it knows what it tried to send, and what Slave<br />

received). If noise rate is too high (over 25%) with high probability there is an<br />

Eavesdropper and data transmission is aborted. Slave calculates noise level (it<br />

knows what Master tried to send and what it received). If noise rate is too high<br />

(over 25%) with high probability there is an Eavesdropper and data transmission is<br />

aborted. The data is sent using Vernam chippering with the BB84 key on a Classic<br />

public channel. The Slave Station stores and <strong>de</strong>co<strong>de</strong>s the ciphered message with the<br />

BB84 secret, private & secure key (Fig. 2).<br />

5. Implementing the BB84 protocol in a stu<strong>de</strong>nt oriented experimental<br />

apparatus<br />

5.1. Background<br />

The experimental setup will follow the initial i<strong>de</strong>a that was used in the Optical<br />

Institute <strong>of</strong> Orsay, France. In that case, the photons were transmitted between two<br />

windows <strong>of</strong> two separate buil<strong>din</strong>gs. For co<strong>din</strong>g the qubits the experiment used the<br />

four polarization states (horizontal, vertical, circular left and circular right).<br />

Physically, they were created by applying a voltage on an electro-optical modulator.<br />

The qubit sequence resulting from the co<strong>de</strong>d polarization is generated by hardware<br />

means, by using two Fibonacci configured linear registries. Each registry has an<br />

20<br />

output <strong>of</strong> 2 1 bits, and the 4 states <strong>of</strong> the protocol suffer 2-bit co<strong>din</strong>g, each <strong>of</strong> the<br />

bits being a part <strong>of</strong> a pseudo-random sequence. For minimizing diffraction effects, the<br />

radius <strong>of</strong> the photon beam is exten<strong>de</strong>d to 2 cm, by using a two-lens system, before<br />

being transmitted 30 m through open air. The photons are collected by Bob through<br />

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the same system, at which 4 avalanche photo-dio<strong>de</strong>s were ad<strong>de</strong>d. Measurements <strong>of</strong><br />

polarization were ma<strong>de</strong> by selecting the states, as the photons are either transmitted or<br />

reflected by a beam splitter at the inci<strong>de</strong>nce angle <strong>of</strong> 45°. Horizontal and vertical<br />

states were created by the beam splitter, while the circular left and right states were<br />

separated by a special splitter that converts circular polarization into linear<br />

polarization, and then discern them through the same splitting method.<br />

5.2. The efficiency <strong>of</strong> the single photon source and the Poisson statistics<br />

Primary characteristics <strong>of</strong> the single photon source quality ma<strong>de</strong> by Alice consist <strong>of</strong><br />

measuring the single and multi-photon emission probabilities, compared with weak<br />

coherent pulses (WCP), with the same amount <strong>of</strong> photons per pulse. For a<br />

4<br />

transmission sequence <strong>of</strong> 0.2 s and pulse frequency <strong>of</strong> 5.3 MHz, a total <strong>of</strong> 8.8<br />

10<br />

photons are recor<strong>de</strong>d by Alice. By correcting the efficiency <strong>of</strong> the photo-dio<strong>de</strong>s<br />

(APD) APD<br />

0.6 the global efficiency adds up to 2.8%. After passing through the<br />

modulator, characterized by TEOM<br />

0.9 and Toptic<br />

0.94 , the mean <strong>of</strong> the sent<br />

photons per pulse was 0.0235 . Reduction <strong>of</strong> the multi-photon emissions can be<br />

set in Alice's part <strong>of</strong> apparatus. Photon statistics can be counted precisely by Bob's<br />

measurements, thus resulting in the distribution <strong>of</strong> the photon numbers. Evaluations<br />

6<br />

were carried out on 40 10 pulses recor<strong>de</strong>d by Bob [1]. For a time sample, <strong>de</strong>tection<br />

3<br />

6<br />

probabilities for a photon or photon pair are P1 d<br />

7.610<br />

and P2 d<br />

2.7 10 .<br />

Configuration <strong>of</strong> the photo-dio<strong>de</strong>s shows that the <strong>de</strong>tection probability P2d<br />

is 5/8 <strong>of</strong><br />

the reception probability <strong>of</strong> the same pair, while the probability that a photon pair<br />

falls on the same photo-dio<strong>de</strong> is <strong>of</strong> 3/8. The reduction factor is given by:<br />

2<br />

5 P1<br />

d<br />

R 6.7 . This result is in accordance with the Poisson distribution, and<br />

8 2P2<br />

d<br />

thus can be used in further calculus. Information leak to an intru<strong>de</strong>r connected to the<br />

( m)<br />

quantum channel is S , which shows the probability that a photon leaves Alice's<br />

( m) 4<br />

system. For an equivalent WCP we have S 1 (1 ) e 2.7 10<br />

, while for<br />

WCP<br />

the SPS<br />

( m) 1 [1 (1 ) ] 4.1 10<br />

5<br />

SSPS<br />

e [4].<br />

6.7<br />

5.3. Detection probabilities <strong>of</strong> Bob's system<br />

Detection probability <strong>of</strong> Bob's apparatus over a time threshold is<br />

p exp<br />

7.6 10<br />

3<br />

.<br />

Assuming that the absorption <strong>of</strong> the beam is negligible through the 30 m<br />

transmission, and taking into account that the mean 0.0235 , an estimate <strong>of</strong> the<br />

<strong>de</strong>tection apparatus is Bob<br />

0.3 . While measuring photons, errors might appear,<br />

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because <strong>of</strong> unpolarized light. This contributes to compromising the security <strong>of</strong> the<br />

transmission, and <strong>de</strong>crease the maximum transmission distance. By filtering and<br />

spectral insulation, the optical environment can be protected. Measurements were<br />

ma<strong>de</strong> at night time, the probability <strong>of</strong> recor<strong>din</strong>g an incorrect photon per time<br />

5 1<br />

threshold is p 3.8 10 s [4].<br />

dark<br />

6. Our experimental proposal setup<br />

The experiment will take place on a lab table, so there is no need to have<br />

complicated alignment system. A simple laser dio<strong>de</strong> and the transmitter can be<br />

used for alignment, by moving the two supporting legs.<br />

Fig. 2. Experimental proposal.<br />

The experiment consists <strong>of</strong> two main modules: Alice and Bob, in our case,<br />

transmitting and receiving stu<strong>de</strong>nt, that communicate over open air, at the<br />

<strong>de</strong>signated distance for laboratory <strong>of</strong> about 1 m.<br />

The classical channel is a basic TCP/IP connection (coaxial or UTP cable). The<br />

experiments for optical fibers transmissions are also consi<strong>de</strong>red.<br />

6.1. Transmitter Module<br />

Fig. 3. The Alice module.<br />

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The module is <strong>de</strong>signed to produce a stream <strong>of</strong> single polarized photons accor<strong>din</strong>g<br />

to the choice <strong>of</strong> basis and bit value. Because no source can produce single<br />

photons, we use pulses that have the property <strong>of</strong> coherency. They are called weak<br />

coherent pulses (WCP), <strong>of</strong> Poisson distribution and mean photon number<br />

0.0235 . To produce the pulses, we will use four laser dio<strong>de</strong>s, oriented around<br />

a conical mirror at the <strong>de</strong>sired polarization angles. The polarization problem is<br />

solved by the laser dio<strong>de</strong>s, that have intrinsic polarization. After the beams are<br />

reflected by the conical mirror, they pass a spatial filter, which consists <strong>of</strong> two<br />

100 m at 0.9 cm apart. It serves a special purpose, that <strong>of</strong> making the pulse from<br />

the four dio<strong>de</strong>s indistinguishable from the others, in spatial terms. This measure<br />

has to be taken because without the spatial filtering, the co<strong>de</strong> can be broken quite<br />

easily. In or<strong>de</strong>r to get as much light as possible through the spatial filter, there is a<br />

lens with a focal length f = 2.75 mm between the conical mirror and the pinholes<br />

<strong>of</strong> the spatial filter. Because <strong>of</strong> the very strong spatial filtering, the alignment <strong>of</strong><br />

the pinholes is crucial, otherwise the <strong>de</strong>sired mean photon count will not be<br />

achieved for all polarizations. [4]<br />

6.2. Receiver Module<br />

Fig. 4. Receiver module schematic.<br />

The module is the heart <strong>of</strong> the receiver unit is connected directly to a receiver lens<br />

and a spatial filter (SF), that are positioned so that the transmitted beam is focused<br />

on the primary <strong>de</strong>vice <strong>of</strong> the module. The primary <strong>de</strong>vice is an interference filter<br />

with a red color glass filter. This is important to allow for daylight operation,<br />

because it rejects stray light, while permitting polarized light to pass. The<br />

remaining optical <strong>de</strong>vices divi<strong>de</strong> the photon beams into bases H/V and +/-, the<br />

construction being based on the i<strong>de</strong>a by John Rarity and Paul Tapster. An inci<strong>de</strong>nt<br />

photon sees the 50/50 beam splitter (BS). If it is reflected it will see the polarizing<br />

beam splitter(PBS) <strong>of</strong> the photon in the H/V basis, which in combination with the<br />

two silicon avalanche photo dio<strong>de</strong>s (APD) H and V. If APD V <strong>de</strong>tects a photon it<br />

is supposed to be in the V basis, whereas if APD H <strong>de</strong>tects a photon, it is<br />

supposed to be in the H basis.<br />

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102 Paul Sterian, Andreea Rodica Sterian<br />

Any photon that is transmitted through the beam splitter passes through a half-wave<br />

plate, set at an angle <strong>of</strong> 22.5, so that it rotates the linear polarization by 45 <strong>de</strong>grees.<br />

Afterwards, a +45 <strong>de</strong>grees polarized photon is <strong>de</strong>tected by APD 1 and converted into<br />

the horizontal basis H, while a - 45 <strong>de</strong>grees polarized photon is <strong>de</strong>tected by APD 3<br />

and converted into the vertical basis V. Whenever a photon is measured in the wrong<br />

basis, the measurement outcome is completely random. The APD-s have to be cooled<br />

in or<strong>de</strong>r to reduce dark counts, at a temperature between - 25 and - 10 <strong>de</strong>grees. To<br />

reach these temperatures, the photo-dio<strong>de</strong>s are put into an aluminum block which is<br />

cooled by a Peltier element glued to it from below [4]. The bit error rate (BER) [6] for<br />

each channel was estimated from data taken during key exchange. It is given by the<br />

Nwrong<br />

expression: BER , where N wrong is the number <strong>of</strong> bits in error and N total is the<br />

Ntotal<br />

number <strong>of</strong> bits received in total. This gives a measure <strong>of</strong> the likelihood <strong>of</strong> receiving a<br />

zero when a one was sent from the transmitter. All but one <strong>of</strong> the BER values in table<br />

1 are sufficiently low showing that optical imperfections from the equipment will<br />

contribute little to the error in the sifted key. The system will operate in natural light<br />

and artificial light in the lab, thus the background error rate must be consi<strong>de</strong>red. This<br />

is a factor that could limit the entire experimental setup. We start from the signal<br />

RMT <br />

count for this rig [8]: S , where R is the repetition rate, M is the average<br />

4<br />

number <strong>of</strong> photons per pulse, T is the lumped transmission and η is the <strong>de</strong>tection<br />

efficiency <strong>of</strong> Bob's APDs. The product is divi<strong>de</strong>d by 4 because there are 4 <strong>de</strong>tectors<br />

(or 4 polarization states). The background rate is given by Pb<br />

Bt , where B is the<br />

background the background count rate per APD and t is the time synchronization<br />

gate. Half the counts induce errors and half <strong>of</strong> there are thrown away. The error<br />

Pb<br />

rate is: E Ebase<br />

. E must be less the 0.07 therefore the maximum acceptable<br />

S<br />

MT<br />

background rate is: B . In consi<strong>de</strong>ring the system presented here,<br />

75.5t<br />

estimates can be ma<strong>de</strong> for the following values [8]:<br />

1. M ~ 0.3, an accepted value for guaranteed security <strong>of</strong> low loss systems.<br />

2. T ~ 1 since the source can be imaged on to the receiver and the system is<br />

short range and thus atmospheric loss is negligible.<br />

3. η ~ 0.045 taking into account the quantum efficiency <strong>of</strong> the <strong>de</strong>tectors and the<br />

presence <strong>of</strong> the narrow band filter and polarizers.<br />

4. t = 5 ns gate synchronization time.<br />

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Implemented in a Stu<strong>de</strong>nt Laboratory 103<br />

Thus the maximum background count rate per <strong>de</strong>tector can be given as roughly<br />

B 36000 counts/s. In this system, the data is recor<strong>de</strong>d first during the quantum<br />

transmission and processed afterwards in a few seconds. The start <strong>of</strong> the<br />

transmission is <strong>de</strong>termined approximately by searching for a jump in the<br />

frequency <strong>of</strong> time tags as Bob starts measuring before Alice begins her<br />

transmission. Alice transmits sub-5 ns pulses every 200 ns, therefore a time<br />

synchronization gate <strong>of</strong> 5 ns reduces the probability <strong>of</strong> registering a background<br />

event within the gate by a factor <strong>of</strong> 40 [8]. The clock at the receiver is thus<br />

synchronized with the clock at the transmitter by searching for time tags that sit at<br />

separations <strong>of</strong> 200 ns and adjusting the time separation slightly every ~100 ms to<br />

compensate for clock drift. The advantage <strong>of</strong> this set-up is that no timing<br />

reference signal is nee<strong>de</strong>d. To <strong>de</strong>termine the exact start time <strong>of</strong> the data, the<br />

receiver reveals a random subset <strong>of</strong> his measured bit values and the basis he used<br />

to the transmitter. The transmitter then finds the data start by performing a sparse<br />

correlation against her stored data. This random subset can also be reused to<br />

estimate the error rate.<br />

Fig. 5. Full experimental rig.<br />

It should be noted that our implementation <strong>of</strong> error correction requires that the two<br />

parties both generate the same random factor graph. Once both <strong>of</strong> them know the<br />

number <strong>of</strong> message bits they are error correcting over, and the measured error rate,<br />

they seed a pseudo-random number generator from their OTP and use this to generate<br />

an appropriate factor graph.<br />

The eavesdropper, is assumed not to know which <strong>of</strong> the 2 256 , say, different factor<br />

graphs the communicating parties are using [8].<br />

For implementing this type <strong>of</strong> encryption we also can use fiber optics, as used in<br />

“Clavis” [9, 10] <strong>de</strong>vices for BB84 co<strong>de</strong> implementation.<br />

Fiber optics may provi<strong>de</strong> a much longer distance for light propagation, thus<br />

facilitating the wi<strong>de</strong> area implementation for this type <strong>of</strong> secured data<br />

transmissions.<br />

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104 Paul Sterian, Andreea Rodica Sterian<br />

7. Improving BB84 by using photon echo<br />

Our optical channel can be improved using the photon echo effect [3]. The co<strong>de</strong><br />

encrypting can be ma<strong>de</strong> by introducing a supplementary key if we use the photon<br />

echo. We have three states associated to the 1 and 0 qubits that are available for<br />

encrypting. That correspond to the possibility <strong>of</strong> associating to the two input<br />

impulses two or three output impulses, the third one correspon<strong>din</strong>g to the photon<br />

echo, generated after an algorithm or by our own will. Excitement <strong>of</strong> super radiant<br />

states by irradiating a probe with an coherent optical impulse, with its duration<br />

and intensity conveniently chosen can be shown with the photon echo [3]. In<br />

principle, we consi<strong>de</strong>r the exciting <strong>of</strong> a ruby crystal, for example, with two<br />

coherent, i<strong>de</strong>ntical optical impulses A and B (emitted by a ruby laser), having a<br />

duration <strong>of</strong> ∆t (ns), the <strong>de</strong>lay <strong>of</strong> B impulse when passing through the probe, will<br />

be ∆T ∆t, showing in the figure 6 [12, 13].<br />

Fig. 6. Principle <strong>of</strong> photon echo.<br />

We can see at the exit, besi<strong>de</strong> the two impulses A' and B', which correspond to the<br />

emitted impulses A and B, a third impulse A'', symmetrical positioned to A' and<br />

B', named photon echo [3]. For explaining the photon echo, we use the precession<br />

equation, for a circular polarized radiation field, in a reference system which<br />

d 0<br />

rotates round the z axis with the frequency ω: P P ( Ei<br />

k .<br />

dt<br />

<br />

Due to the unequal width <strong>of</strong> the transition frequency for ruby atoms, and due to the<br />

local field, variation, P and ω 0 will be affected by in<strong>de</strong>x k , which <strong>de</strong>fines the k atom.<br />

If before applying impulse A, the atoms were all in the fundamental state, the<br />

vector<br />

P<br />

N<br />

P is oriented in the negative direction <strong>of</strong> z axis. Applying the A<br />

k1<br />

k<br />

impulse, <strong>of</strong> E a amplitu<strong>de</strong>, between t = 0 and t = ∆t, a precession movement <strong>of</strong> P<br />

around the pseudo field appears. If E / 0<br />

X , the procession is ma<strong>de</strong><br />

A<br />

around the x axis with an X E a ∆t angle so for an intensity <strong>of</strong> the impulse that<br />

satisfies the condition X E a ∆t = π/2 (π/2 impulse), P will be orientated after y<br />

axis in t = ∆t, the system being in a superradiant state Δ.<br />

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Applications <strong>of</strong> Quantum Cryptology for Data Transmissions<br />

Implemented in a Stu<strong>de</strong>nt Laboratory 105<br />

Fig. 7. Superradiance states.<br />

When the E a field stops, the atoms will execute precession movement with different<br />

speeds around the pseudo-field<br />

k where . During these movements<br />

X<br />

0k<br />

in t = ∆t and t = ∆t + ∆T interval, Pk<br />

components will be <strong>de</strong>phased so P<br />

diminishes [3]. B impulse which applies in the moment t = ∆t + ∆T must reflect the<br />

P vectors in the xy plane, reported to the x axis. To obtain this effect the following<br />

k<br />

condition must apply: η E b ∆t = π (π impulse), meaning that IB<br />

4IA, I<br />

A<br />

and I<br />

B<br />

specifying the two impulses intensities. In the interval t = 2 ∆t + ∆T and<br />

t = 2 (∆t + ∆T) the vectors P are moving like in the <strong>de</strong>phase interval, getting in<br />

k<br />

phase after another interval equal to ∆T. The correspon<strong>din</strong>g state <strong>of</strong> the vectors<br />

'<br />

in rephasing is a superradiant state, highlighted by echo impulse emission A<br />

E<br />

[3].<br />

We can use the photon echo to improve the co<strong>de</strong> by ad<strong>din</strong>g either a controlled error<br />

on the channel or transforming the channel from a binary channel to a ternary<br />

channel. A ternary channel is more efficient in transmitting co<strong>de</strong>d information but in<br />

this form the ternary channel will be created on a binary one, using the echo to create<br />

the third channel <strong>of</strong> communication. We also can improve a channel transmission<br />

width using the photon echo to create a bit <strong>of</strong> data when we want, thus changing the<br />

information meaning and receiving more information that was initially sent.<br />

8. Conclusions<br />

Quantum cryptography implemented with the BB84 protocol <strong>of</strong>fers a high level <strong>of</strong><br />

security for data communications. Although it has not been implemented on a<br />

commercial level, it is suitable for integration in optical fibers communications, with<br />

a wi<strong>de</strong> range <strong>of</strong> applications. Our experimental proposal <strong>of</strong>fers a good stu<strong>de</strong>nt insight<br />

into quantum cryptography, combining the already known and <strong>de</strong>signed modules<br />

Alice and Bob with the potential <strong>of</strong> the photon echo.<br />

P<br />

k<br />

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106 Paul Sterian, Andreea Rodica Sterian<br />

R E F E R E N C E S<br />

[1] Paul Sterian, Dan Alexandru Iordache, Viorica Iordache, "Study <strong>of</strong> the Present Problems <strong>of</strong><br />

the Scientific Information Processing and Transmission'', Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian<br />

Scientists, Series on Science and Technology <strong>of</strong> Information, vol. 3, no. 1, 2010, pp. 101-112.<br />

[2] Dan-Alexandru Iordache, Daniela Radu, Octavian Radu, "Complexity Approach <strong>of</strong> Optical<br />

Communications Systems", Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, Series on Science and<br />

Technology <strong>of</strong> Information, vol. 2, no. 1, 2009, pp. 9-16.<br />

[3] Paul Sterian, “Fotonica”, Editura Printech, Bucuresti 2000, ISBN 973-652-161-3.<br />

[4] Harald Weinfurter and Alfred Laubereau, “Experimental Quantum Cryptography”, 2003,<br />

http://xqp.physik.uni-muenchen.<strong>de</strong>/publ/henning-diplom.pdf.<br />

[5] Id Quantique, Switzerland, “Securing Networks with the Vectis Link Encryptor”,<br />

www.idquantique.com.<br />

[6] Thomas Daniel Jennewein, Anton Zeilinger, “Quantum Communication and Teleportation<br />

using Entangled Photon Pairs”, June 2002, http://www.quantum.univie.ac.at.<br />

[7] Fernando Lucas Rodriguez, QIT IDE.exe,<br />

http://www.fernandolucas.info/QCS, fernandolucas@ieee.org.<br />

[8] J. L. Duligall, M S Godfrey, K A Harrison, W J Munro and J G Rarity, “Low Cost and<br />

Compact Quantum key distribution”, 2006, http://www.iop.org/EJ/abstract/1367-2630/8/10/249.<br />

[9] D.Stucki, N. Gisin, O. Guinnard, G. Ribordy, H. Zbin<strong>de</strong>n, “New Journal <strong>of</strong> Physics 4”,<br />

www.njp.org.<br />

[10] Id 3000 Datasheet v2.1, www.idquantique.com.<br />

[11] Cornel Cobianu, Cazimir Bostan, s.al., “From 2D Microelectronics to 3D Microsystems",<br />

Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, Series on Science and Technology <strong>of</strong> Information,<br />

vol. 3, no. 1, 2010, pp. 31-46.<br />

[12] Ion Apostol, Dan-Alexandru Iordache, Pier Paolo Delsanto, Viorica Iordache, “Study <strong>of</strong> some<br />

Numerical Artifacts Intervening in the Finite Differences Simulations <strong>of</strong> KDV Solitons<br />

Propagation”, Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, Series on Science and Technology<br />

<strong>of</strong> Information, vol. 4, no. 1, 2011, pp. 7-22.<br />

[13] Dana Georgeta Popescu, Paul Sterian, “Nonlinear Interaction Mo<strong>de</strong>ling in Photonic<br />

Crystals”, Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, Series on Science and Technology <strong>of</strong><br />

Information, vol. 4, no. 2, 2011, pp. 105-124.<br />

[14] Sterian Andreea Rodica, “Coherent Radiation Generation and Amplification in Erbium<br />

Doped Systems”, Advances in Optical Amplifiers, Paul Urquhart (Ed.), ISBN: 978-953-307-186-2,<br />

InTech, VIENNA, 2011.<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066-8562 Volume 5, Number 1/2012 107<br />

THE MATHEMATICAL THEORY OF COMMUNICATIONS<br />

VERSUS THE PHYSICAL THEORY OF INFORMATION.<br />

THE UNIVERSE VERSUS THE MULTIVERSE<br />

Dan Alexandru IORDACHE 1<br />

Starting from the “classical” (mathematical) theory <strong>of</strong> information (C. Shannon, W. Weaver), this<br />

work has replaced the <strong>de</strong>finitions <strong>of</strong> the: a) apparent information as a <strong>de</strong>crease <strong>of</strong> the non<strong>de</strong>termination<br />

(uncertainty) <strong>de</strong>gree, by means <strong>of</strong> the overlap area <strong>of</strong> the true and found probability<br />

distributions, respectively, b) agreement <strong>of</strong> a theoretical relation with the experimental data using<br />

the correlation coefficients, by means <strong>of</strong> the error risks at the compatibility rejection, etc., taking<br />

into account also the basic notions <strong>of</strong> the complex systems: (i) the uniqueness parameters, (ii) the<br />

similitu<strong>de</strong> criteria, (iii) the universality classes, (iv) the numerical phenomena intervening in the<br />

computer simulations <strong>of</strong> such systems evolution, etc. [1]. The accomplished analysis pointed out the<br />

existence <strong>of</strong> some surprising co-relations relating the fundamental interactions and particles. The<br />

interpretation <strong>of</strong> these fin<strong>din</strong>gs by means <strong>of</strong> the anthropic principles (lea<strong>din</strong>g to the notion <strong>of</strong> <strong>de</strong>signed<br />

Universe) or by means <strong>of</strong> some recent theoretical mo<strong>de</strong>ls (“<strong>of</strong> quantum gravitation”, “selfreproducing<br />

inflation”, “quantum cosmology with loops”, etc., lea<strong>din</strong>g to Multi-verse mo<strong>de</strong>ls) was<br />

also analysed by this work (see also [2]).<br />

Keywords: Mathematical information theory, Compatibility with experimental results, Complex<br />

systems, Fundamental interactions, Anthropic principles, Theoretical mo<strong>de</strong>ls <strong>of</strong> cosmology<br />

1. Introduction<br />

As it is well-known, after some preliminary works as [3], the mathematical theory<br />

<strong>of</strong> information was rigorously formulated by C. Shannon and W. Weaver [4]<br />

un<strong>de</strong>r the name <strong>of</strong> « mathematical theory <strong>of</strong> communications », and completed by<br />

the works [5] <strong>of</strong> A. J. Khincin, A. N. Kolmogorov, etc. The basic notion <strong>of</strong> this<br />

theory is the so-called uncertainty function H p1 , p2,...<br />

p n associated to the<br />

complete statistical set (collective) C E1 , E2,...<br />

E n <strong>of</strong> incompatible events<br />

E i (i=1, 2, ... n), <strong>of</strong> appearance probability p i . Accor<strong>din</strong>g to the axioms <strong>of</strong><br />

A. J. Khinchin [5] (that allow a rather simple <strong>de</strong>rivation <strong>of</strong> the expression <strong>of</strong> the<br />

uncertainty function), the uncertainty function has properties <strong>of</strong>: 1) symmetry:<br />

H( p2, p1, ... p<br />

n<br />

) = H( p1, p2, ... p<br />

n<br />

), 2) maximum value for the uniform distribution:<br />

1<br />

H( p1, p2, ... p<br />

n<br />

) = maximum for: p1 p2<br />

... pn , 3) prolongation:<br />

n<br />

H( p1, p2, ... p<br />

n<br />

,0) = H( p1, p2, ... p<br />

n<br />

), i.e. the addition <strong>of</strong> an impossible event (<strong>of</strong> null<br />

probability) does not change the value <strong>of</strong> the uncertainty function, 4) continuity: the<br />

function H( p1, p2, ... p<br />

n<br />

) has to be continuous relative to its variables:<br />

1 Pr<strong>of</strong>essor, Physics Department, University “Politehnica” <strong>of</strong> Bucharest, Romania; Honorary Member<br />

<strong>of</strong> Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists, Section <strong>of</strong> Information Science and Technology (IT).<br />

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108 Dan Alexandru Iordache<br />

1 , 5) linearity: HC C'<br />

H(<br />

C)<br />

p HC'<br />

, where H ( C C' )<br />

p , p2,...<br />

p n<br />

and C<br />

E <br />

n<br />

i1<br />

i E i<br />

i<br />

E i E ' j =<br />

Cartesian product <strong>of</strong> the statistical collectives C and C’, and to the statistical<br />

collective C’, in conditions when the event E i appeared.<br />

H ' are the uncertainty functions correspon<strong>din</strong>g to the set <br />

It was found [5] that the uncertainty function H( p1, p2, ... p<br />

n<br />

) fulfilling the above<br />

indicated conditions is: H( p1, p2, ... p<br />

n<br />

) = a <br />

n<br />

p i log b pi<br />

, where a and b are<br />

i1<br />

almost arbitrary constants, that satisfy the conditions: a > 0 and b > 1. One finds so<br />

that the uncertainty function H( p1, p2, ... p<br />

n<br />

) represents the average (theoretical)<br />

value <strong>of</strong> the so-called information entropy, <strong>de</strong>fined by the relation:<br />

Si<br />

a<br />

logb<br />

pi<br />

(1)<br />

Similarly, for the continuous statistical collectives (<strong>de</strong>scribed by the probability<br />

<strong>de</strong>nsity p(x)), the uncertainty function is given by the expression:<br />

<br />

H( p(<br />

x))<br />

a<br />

p(<br />

x)logb ( p(<br />

x)<br />

x)<br />

dx [where Δx is the (conveniently chosen)<br />

<br />

“quantum” <strong>of</strong> the variable x] and the information entropy by the expression:<br />

S( p(<br />

x))<br />

a<br />

log<br />

b ( p(<br />

x)<br />

x)<br />

. (2)<br />

therm. B<br />

We have to un<strong>de</strong>rline also that the expression (2) is absolutely similar to the<br />

(previous) Planck-Boltzmann expression: S k<br />

ln<br />

<strong>of</strong> the thermodynamic<br />

entropy (k B is the Boltzmann’s constant, while stands for the<br />

probability <strong>de</strong>nsity <strong>of</strong> micro-states localisation in the phases’ space).<br />

2. Logical scheme <strong>of</strong> the humankind information accumulation<br />

It is well known that the information processing and storage abilities <strong>of</strong> each<br />

individual people brain are drastically limited. For this reason, the humankind<br />

advance in its race for the complex systems knowledge and use imposes the<br />

strong cooperation <strong>of</strong> the human beings by information transmission. Taking into<br />

account that the information transmission is a resonance process (see fig. 1), it is<br />

necessary to ensure: a) the obtained (got) information (see fig. 2) cleaning before<br />

a new experiment (measurement, embryo <strong>de</strong>velopment, Universe genesis, etc.),<br />

b) a sufficiently broad and well-located information receiver bell, c) an implant<br />

(insi<strong>de</strong> the information receiver bell) <strong>of</strong> several connecting relays, achieving the<br />

cross-fertilization between the information source(s) and its virtual applications,<br />

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Universe versus Multiverse 109<br />

so that « Toute la suite <strong>de</strong>s hommes <strong>de</strong>puis le cours <strong>de</strong> tant <strong>de</strong> siècles est comme<br />

un seul homme qui vit toujours et qui apprend continuellement » (Blaise Pascal).<br />

Fig. 1. Information transmission as a resonance process. Fig. 2. Magnetic memory –<br />

example <strong>of</strong> got information.<br />

3. Main Conceptual Differences between Mathematics and Nature Sciences<br />

3.1. Typical elementary object<br />

While in Mathematics the typical elementary object (the problem unknown) is a<br />

well-<strong>de</strong>fined number or segment, in Nature Sciences this elementary object is a<br />

parameter , <strong>de</strong>scribed by a certain probability distribution P(p) <strong>of</strong> the individual<br />

values p (see figure 3).<br />

While the value <strong>of</strong> the unknown <strong>of</strong> a mathematical problem with a right<br />

formulation is obtained exactly by means <strong>of</strong> the problem solution, the most<br />

probable individual value (named also “true value”, or “mathematical hope”) t p<br />

<strong>of</strong> the physical parameter p cannot be never exactly obtained!<br />

For this reason, the <strong>de</strong>finition <strong>of</strong> the real information amount has to be given by<br />

means <strong>of</strong> the overlap area <strong>of</strong> the normalised to 1 probability distribution functions<br />

correspon<strong>din</strong>g to measurements and to the true parameter, respectively (fig. 4).<br />

Fig. 3. Probability distribution<br />

<strong>of</strong> a parameter p individual values.<br />

Fig. 4. Definition <strong>of</strong> the true information amount<br />

obtained by measurements.<br />

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110 Dan Alexandru Iordache<br />

3.2. Uniqueness parameters<br />

While the number <strong>of</strong> the uniqueness parameters <strong>of</strong> a mathematical problem is<br />

fixed [e.g.: 3 for an arbitrary triangle (the lengths <strong>of</strong> the 3 si<strong>de</strong>s, or the lengths <strong>of</strong> 2<br />

si<strong>de</strong>s and the angle between them, etc.)], the number <strong>of</strong> the uniqueness<br />

parameters <strong>of</strong> a physical system <strong>de</strong>pends on the required accuracy for the<br />

consi<strong>de</strong>red system <strong>de</strong>scription [e.g., the thermodynamic state <strong>of</strong> the air is<br />

<strong>de</strong>scribed by: (i) only 2 parameters (usually the temperature and the pressure) in a<br />

first or<strong>de</strong>r approximation, (ii) by 3 physical parameters (ad<strong>din</strong>g e.g. the humidity)<br />

in the frame <strong>of</strong> a better approximation, (iii) 4 physical parameters (ad<strong>din</strong>g also the<br />

carbon dioxi<strong>de</strong> content) in the frame <strong>of</strong> a still better approximation, etc.<br />

3.3. Well-formulated problems<br />

While in mathematics a well-formulated problem corresponds usually to a system<br />

<strong>of</strong> compatible and non-redundant equations, the number <strong>of</strong> this system equations<br />

being equal to the number <strong>of</strong> unknowns <strong>of</strong> the mathematical problem, in nature<br />

sciences a well-formulated problem corresponds to a system <strong>of</strong> (slightly)<br />

incompatible (and non-redundant) equations, and the number <strong>of</strong> equations has to<br />

be consi<strong>de</strong>rably larger than that <strong>of</strong> unknowns. This fact is due to the fluctuations<br />

<strong>of</strong> the individual values <strong>of</strong> the physical parameters and even to the presence <strong>of</strong><br />

some hysteretic behaviour (the individual values could <strong>de</strong>pend on the system<br />

previous history) <strong>of</strong> the physical systems.<br />

3.4. Position <strong>of</strong> the incomplete induction method<br />

While in mathematics the incomplete induction method represents only the first<br />

step towards the inference (particularly, by the complete induction method) <strong>of</strong> a<br />

theorem, in Physics this (incomplete induction) method represents an essential<br />

method, because it allows the discovery <strong>of</strong> some truths which are not equivalent to<br />

the information set used to formulate the respective hypothesis. The incomplete<br />

induction method represents one <strong>of</strong> the most fertile methods used by the nature<br />

sciences for the i<strong>de</strong>ntification <strong>of</strong> some new plausible hypotheses and the<br />

subsequent discovery <strong>of</strong> some new physical phenomena and laws.<br />

4. On the bridge between the mathematical theory <strong>of</strong> communications<br />

(information) and the physical theory <strong>of</strong> information<br />

For a uniform distribution <strong>of</strong> the true value t X insi<strong>de</strong> its correspon<strong>din</strong>g confi<strong>de</strong>nce<br />

interval:<br />

1<br />

<br />

~ xn<br />

zLs( ~ xn<br />

)<br />

~<br />

n<br />

L<br />

( ~ X<br />

x z s xn<br />

)<br />

p ( t ) da C<br />

dt 2C<br />

z s( ~ x ),<br />

X<br />

X<br />

hence the correspon<strong>din</strong>g expression <strong>of</strong> the uncertainty function is:<br />

L<br />

n<br />

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Universe versus Multiverse 111<br />

<br />

2z<br />

s x <br />

H p t a<br />

p t p t x<br />

dt a L ( ~ n)<br />

( ( X )) ( X ) logb<br />

( ( X ) ) X logb<br />

<br />

. (3)<br />

x<br />

<br />

<br />

It results that the apparent information obtained in frame <strong>of</strong> the n th physical<br />

<strong>de</strong>termination can be expressed by means <strong>of</strong> the square mean errors correspon<strong>din</strong>g<br />

to the sets <strong>of</strong> the obtained results obtained after the (n-1) <strong>de</strong>termination and after<br />

the n th <strong>de</strong>termination as:<br />

<br />

I<br />

n<br />

app n Hn<br />

Hn<br />

a 1<br />

. 1 log<br />

<br />

b .<br />

n<br />

One finds so that the usual I app.n > 0 values (correspon<strong>din</strong>g to the convergence towards<br />

the true value), it is possible to meet also values I app.n < 0, which could be due to:<br />

a) rough errors (hence misinformation),<br />

b) random gathering <strong>of</strong> the first individual values, the <strong>de</strong>cision being<br />

established by means <strong>of</strong> some statistical tests.<br />

It results that the additional elements brought by the physical theory <strong>of</strong><br />

information refer mainly to: (i) experimental measurements, (ii) the correspon<strong>din</strong>g<br />

errors, (iii) the necessary statistical tests.<br />

For this reason, the compatibility <strong>of</strong> a given theoretical relation y = f(x) with a certain<br />

set <strong>of</strong> experimental individual values pairs x s , y s (s=1, 2, … N) should be <strong>de</strong>ci<strong>de</strong>d not<br />

starting from the usual correlation coefficient which does take into account the<br />

existing experimental errors, but from the error risks at the compatibility rejection <strong>of</strong><br />

p<br />

each “suspect” pair x s , y s :<br />

<br />

s<br />

qs exp <br />

, where (see also fig. 5):<br />

2<br />

<br />

2 1<br />

r <br />

p<br />

s<br />

xs<br />

x <br />

<br />

( x)<br />

<br />

~ 2<br />

2<br />

y <br />

~<br />

s y <br />

<br />

( y)<br />

<br />

x <br />

~<br />

s x<br />

2r<br />

<br />

( x)<br />

<br />

<br />

<br />

y <br />

~<br />

s y <br />

. (4)<br />

( y)<br />

<br />

Fig. 5. Evaluation procedure <strong>of</strong> the error risk at the compatibility rejection<br />

<strong>of</strong> a theoretical relation Y = f(X) relative to some local data.<br />

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112 Dan Alexandru Iordache<br />

5. Main features <strong>of</strong> the complex systems <strong>de</strong>scription<br />

Because several completely different complex systems [computer arrays, robots,<br />

networks, social sciences, biology (with some specific topics: colonies, swarms,<br />

immunology, brain, genetics, proteomics), non-linear dynamics, economics,<br />

mathematics, glasses, agents, cognition, etc.] have some common features centred<br />

on their statistical behaviour and the correspon<strong>din</strong>g phase transforms [6], [7], it<br />

results that these complex systems have certain universality properties, which –<br />

due to their generality (see e.g.[7a]) - can be <strong>de</strong>scribed only by some specific<br />

numbers (the so-called similitu<strong>de</strong> numbers, or criteria [8]).<br />

nU <br />

If: P <br />

i Ui , where [P] is the physical dimension <strong>of</strong> a parameter P specific<br />

i1<br />

to the studied state (or process), then 2 states (or processes) Σ’, Σ” are named<br />

similar if the values <strong>of</strong> the parameters U i | i 1,<br />

n<br />

and P correspon<strong>din</strong>g to these<br />

P'<br />

' "<br />

states fulfil the relation [8]: i<br />

n U<br />

U i U i . Some <strong>of</strong> the uniqueness<br />

P"<br />

i1<br />

parameters could be similitu<strong>de</strong> criteria, i.e. non-dimensional parameters: [s] = 1,<br />

with equal values: s’ = s” in all similar states or processes. While the first known<br />

similitu<strong>de</strong> criterion was introduced by Archime<strong>de</strong>s (287-231 b. Chr.):<br />

3<br />

<br />

Ar gl , the first (existence) theorem <strong>of</strong> the similitu<strong>de</strong> theory was stated by<br />

2<br />

<br />

Newton, all these theorems being presented in work [9].<br />

<br />

Fig. 6. Plots <strong>of</strong> different pseudo- convergent<br />

simulations <strong>of</strong> elastic pulses propagation.<br />

Fig. 7. Gradual installation <strong>of</strong> instability in<br />

simulations <strong>of</strong> elastic pulses propagation.<br />

The accomplished study [1] <strong>of</strong> the typical study procedure <strong>of</strong> complex systems<br />

pointed out that it involves the following main stages: a) i<strong>de</strong>ntification <strong>of</strong> the<br />

uniqueness parameters, b) i<strong>de</strong>ntification <strong>of</strong> the characteristic similitu<strong>de</strong> criteria, c)<br />

obtainment <strong>of</strong> the set <strong>of</strong> irreducible criteria, d) translation <strong>of</strong> all relations <strong>of</strong><br />

scientific and/or technical interest in terms <strong>of</strong> similitu<strong>de</strong> criteria, e) check <strong>of</strong> the<br />

theoretical and experimental similitu<strong>de</strong> mo<strong>de</strong>ls, f) test <strong>of</strong> compatibility <strong>of</strong><br />

theoretical relations and mo<strong>de</strong>ls relative to the existing experimental data.<br />

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Universe versus Multiverse 113<br />

Fig. 8. Distortions in the simulations <strong>of</strong> some random walk processes [10].<br />

6. Main numerical phenomena intervening in the Data Processing<br />

A <strong>de</strong>tailed study <strong>of</strong> the main numerical phenomena: pseudo-convergence (fig. 6),<br />

instability (fig. 7), distortions (fig. 8), intervening in the computer evaluations <strong>of</strong><br />

certain physical parameters and/or some simulations <strong>of</strong> different physical<br />

phenomena was accomplished by work [10].<br />

Taking into account the various errors types and numerical phenomena<br />

intervening in the data processing, we consi<strong>de</strong>r as the most accurate data<br />

processing procedure that presented in the frame <strong>of</strong> fig. 9.<br />

Fig. 9. Basic Stages <strong>of</strong> the present Scientific Information Processing.<br />

7. Interpretation <strong>of</strong> the physical information about Complex Systems<br />

Unlike the classical (mathematical) information, the physical information (referring to<br />

complex systems, especially) requires a very careful interpretation. First <strong>of</strong> all, it is<br />

necessary to answer to the basic questions about the observed features:<br />

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114 Dan Alexandru Iordache<br />

a) are they random or reproducible?<br />

b) could they be connected to other results, obtained by different methods?<br />

c) could they be explained by natural causes or it seems to intervene some<br />

transcen<strong>de</strong>nt reasons?<br />

We have to un<strong>de</strong>rline that the acceptance <strong>of</strong> a physical interpretation needs<br />

multiple completely different experimental results, whose explanations converge<br />

to this interpretation. E.g., the existence and parameters (charge, mass) <strong>of</strong><br />

electrons were established as a result <strong>of</strong> AT LEAST 5 completely different<br />

experiments:<br />

(i) the electrolysis (Faraday’s) laws lea<strong>din</strong>g to the elementary electrical charge<br />

e = F/N,<br />

(ii) the J.J. Thomson’s experiment concerning the cathodic rays <strong>de</strong>viations in<br />

an electrical field, which pointed out the existence <strong>of</strong> the electron,<br />

(iii) the Millikan’s experiment which led to the electrical charge <strong>of</strong> the<br />

electron,<br />

(iv) the Lenard’s method <strong>of</strong> crossed (electrical and magnetic) fields, which<br />

allowed the evaluation <strong>of</strong> the specific charge e/m <strong>of</strong> the electron,<br />

(v) the Compton’s effect which allowed the evaluation <strong>of</strong> the rest mass <strong>of</strong> the<br />

electron.<br />

Without redundant (completely different) experimental methods, the Physics is<br />

<strong>of</strong>ten subject to major errors; some recent examples:<br />

a) the so-called anomalons (1970-1980), erroneous interpretation supported<br />

initially by several very good Physics reviews,<br />

b) the so-called ”fusion nuclear reactions at low temperatures” (Palladium<br />

compounds, 1980-1990), again a mis-interpretation,<br />

c) the trans-uranium 118 element, initially claimed by a research group <strong>of</strong> the<br />

Berkeley University and vanished after 2-3 years.<br />

For this reason, the interpretation <strong>of</strong> some new Physics experiments has to be<br />

cautiously examined; some examples:<br />

(i) the Palo Alto results concerning the ”magnetic monopoles” and the ”exotic<br />

particles”, generally,<br />

(ii) the very recent (2011) results <strong>of</strong> Pamela’s orbital station, referring to the<br />

anomalous strong fluxes <strong>of</strong> accelerated cosmic radiations around our planet,<br />

which seem to indicate that the Earth has an absolutely singular location in our<br />

(Milky Way) galaxy, etc.<br />

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Universe versus Multiverse 115<br />

8. Just Six Numbers seem be able to <strong>de</strong>scribe the Universe structure [12].<br />

The Anthropic principle(s) [15]<br />

In 1937, the British Physics Nobel prize laureate Paul A. M. Dirac had noted that the<br />

number <strong>of</strong> baryons (basically protons plus neutrons) in the universe (~ 10 77 ) is almost<br />

equal to the inverse square <strong>of</strong> the gravitational coupling constant<br />

<br />

2<br />

<br />

<br />

k m p<br />

39<br />

C 5.90610<br />

<br />

<br />

g<br />

[11]. Later it was found that amazingly the<br />

c<br />

<br />

<br />

<br />

electromagnetic intersection parameters are also strongly connected to the basic<br />

quantum parameters, the electromagnetic coupling constant ( o being the vacuum<br />

2<br />

eo<br />

e o 1<br />

electromagnetic impedance): Ce<br />

being also given by a<br />

c 2h<br />

137.036<br />

transcen<strong>de</strong>nt number (the so-called Sommerfeld’s fine structure constant). The<br />

synthesis <strong>of</strong> the results obtained during the last <strong>de</strong>ca<strong>de</strong>s indicates that a set <strong>of</strong> only 6<br />

numbers is able to <strong>de</strong>scribe the Universe structure. These « constitutive » constants<br />

may be chosen: a) starting from the 4 fundamental interactions coupling constants C s<br />

1<br />

≈ 1, C e , that <strong>of</strong> the weak nuclear interactions C w ≈ 3·10 -7 and the<br />

137.036<br />

gravitational one C g ≈ 5.90610 -39 , and ad<strong>din</strong>g the ratio <strong>of</strong> rest-masses <strong>of</strong> the<br />

proton and electron: m op /m oe 1836.15 and the number <strong>of</strong> physical dimensions <strong>of</strong><br />

the Universe: D = 4 (usually) and D = 10 or 11 around the Planck’s time t P <br />

0.53310 -43 s, characteristic to the ”Big Bang” process, b) by means <strong>of</strong> the<br />

M. Rees [12] parameters: (i) the relative strength <strong>of</strong> the electric coupling constant<br />

to the gravitational one: C emg /C g 1.235610 36 , (ii) the nuclear efficiency (percent<br />

<strong>of</strong> the mass <strong>of</strong> the nuclear constituents that is converted to heat when they react<br />

via nuclear fusion to form heavier nuclei) 0.007, (iii) the parameter and the<br />

dark matter (known matter 4% <strong>of</strong> the critical mass for Universe to expand<br />

forever), (iv) the cosmological constant (introduced by Einstein in the expression<br />

<strong>of</strong> the Universe acceleration: 3a/R = - 4k( + 3p/c 2 ) + ): 0.7,<br />

(v) proportion <strong>of</strong> energy to their rest mass energy nee<strong>de</strong>d to break up and disperse<br />

clusters: Q 10 -5 , and – <strong>of</strong> course: (vi) the Universe physical dimension(s).<br />

Given being that: a) even in 1961 R.H. Dicke [13] <strong>de</strong>rived that these relations<br />

would imply a narrow time window in the <strong>de</strong>velopment <strong>of</strong> the Universe during<br />

which life could exist, b) some later accomplished calculations [14] seem to<br />

indicate that intelligent life exists only on the earth, it aroused the i<strong>de</strong>a that the earth<br />

too, in addition to the Universe, has experienced divine <strong>de</strong>sign (”anthropic<br />

principle(s)” [15]). We have to un<strong>de</strong>rline that - in opposition to the Anthropic<br />

principle(s) - there appeared very soon (even earlier [16]) some theoretical mo<strong>de</strong>ls<br />

assuming the existence <strong>of</strong> multiple ”parallel” Universes, the so-called Multiverse.<br />

2<br />

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116 Dan Alexandru Iordache<br />

9. Basic Present Cosmological Mo<strong>de</strong>ls lea<strong>din</strong>g to the Hypothesis <strong>of</strong> the<br />

Multiverse existence<br />

In or<strong>de</strong>r to synthesise the basic assumptions and results <strong>of</strong> the main present<br />

cosmological mo<strong>de</strong>ls, Table 1 below presents their basic features.<br />

Table 1. Comparison <strong>of</strong> basic assumptions and results <strong>of</strong> the main present cosmological mo<strong>de</strong>ls<br />

Nr<br />

Theoretical Mo<strong>de</strong>l<br />

Basic<br />

Specific<br />

Number <strong>of</strong><br />

dimensions<br />

t < t Planck t > t Planck Main Authors<br />

1<br />

Quantum<br />

Gravitation<br />

10D Space<br />

1D Time<br />

t ln t<br />

Infinite time<br />

before Big<br />

Bang<br />

Possible 10 500 … 10 1000<br />

parallel Universes,<br />

each with its laws<br />

(L. Susskind,<br />

Stanford U.)<br />

Lee Smolin, Ca [17b]<br />

Th. Damour, Fr;<br />

M. Henneaux,<br />

Be, Solvay;<br />

H. Nicolai, D.<br />

2<br />

Strings<br />

Theory<br />

3D Branes<br />

flowing in a<br />

10D space<br />

10D Space<br />

1D Time<br />

Collisions Big Bang<br />

2001: Neil Turok<br />

(Cambridge, UK)<br />

Paul Steinhardt<br />

(Stanford U.)<br />

3 Black Holes<br />

Compressing<br />

initially<br />

extremely<br />

diluted gas<br />

Compression limit<br />

~ 10 12<br />

Sun masses/ proton<br />

volume<br />

a) Multiple black<br />

holes,<br />

b) Worms holes,<br />

c) Multiverse<br />

(Stephen Hawking)<br />

G. Veneziano<br />

(Coll. Fr.),<br />

M. Gasperini<br />

(U. Bari) >1990<br />

4<br />

Quantum<br />

with loops<br />

Oscillating<br />

Gravitation<br />

Pre-existing<br />

compressing<br />

Universe<br />

Compression limit<br />

~ 10 12<br />

Sun masses/ proton<br />

volume<br />

a) Repulsive<br />

gravitation;<br />

b) Pre-existing<br />

Universe cleaning<br />

(M. Bojowald,<br />

Pennsylv. U.)<br />

A. Ashtekar,<br />

T. Pawlowski,<br />

P. Singh<br />

(Pennsylvania Univ.)<br />

5<br />

Inflation<br />

Theory<br />

A.H. Guth<br />

[18]<br />

Selfreproducing<br />

Inflationary<br />

Universe<br />

10D Space<br />

1D Time<br />

Quantum<br />

Fluctuations <strong>of</strong> the<br />

Scalar Field<br />

Fractal Inflation<br />

12<br />

10<br />

10 times!<br />

(fig. 8) <br />

multiverse<br />

Andrei Lin<strong>de</strong><br />

(U. Stanford) > 1980<br />

[19]<br />

Taking into account that:<br />

a) the present cosmological mo<strong>de</strong>ls represent extrapolations over a huge number<br />

(larger than 25) <strong>of</strong> magnitu<strong>de</strong> or<strong>de</strong>rs <strong>of</strong> the somewhat classical Einstein’s<br />

gravitation and quantum theories, as well as that:<br />

b) the religion (mainly the Bible) predicts some <strong>of</strong> the Universe basic features, the<br />

comparison <strong>of</strong> their arguments in favour <strong>of</strong> the different present basic Universe<br />

evolution mo<strong>de</strong>ls - synthesized by Table 2 - could present a certain interest.<br />

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Universe versus Multiverse 117<br />

Table 2. Comparison <strong>of</strong> the arguments <strong>of</strong> the main types <strong>of</strong> present Universe evolution mo<strong>de</strong>ls<br />

Mo<strong>de</strong>ls type<br />

ARGUMENTS<br />

Multiverse<br />

mo<strong>de</strong>ls<br />

Possible<br />

transcen<strong>de</strong>nt<br />

religions<br />

(mainly,<br />

the Bible)<br />

Theoretical<br />

FAITH (!) in the continuity (over a huge<br />

number <strong>of</strong> magnitu<strong>de</strong> or<strong>de</strong>rs) <strong>of</strong> some<br />

theoretical mo<strong>de</strong>ls<br />

Information (e.g. AND, the Bible, etc.) is<br />

the starting element <strong>of</strong> any <strong>de</strong>sign<br />

(Genesis 1:3-26, John 1:1). AND is<br />

implicitly present in chapters 4 and 5 <strong>of</strong><br />

Genesis.<br />

Experimental Pro<strong>of</strong>s<br />

No one and: a) probably not in future,<br />

outsi<strong>de</strong> our Universe, b) hopes to find<br />

some pro<strong>of</strong>s insi<strong>de</strong> our Universe<br />

Checked experimental evi<strong>de</strong>nce for<br />

some millenary predictions: a) Big Bang<br />

(see fig. 11), b) Relativity, c) Possible<br />

transcen<strong>de</strong>nt relations.<br />

Fig. 10. The Alan Guth’s mo<strong>de</strong>l Fig. 11. Microwave Map <strong>of</strong> the Whole Sky ma<strong>de</strong> from One Year<br />

[18] <strong>of</strong> the Universe evolution. (1992) <strong>of</strong> Data taken by Cosmic Background Explorer-COBE<br />

Differential M.W. Radiometers 10 5 yrs after Big Bang.<br />

10. Transcen<strong>de</strong>nt Integers and possible Transcen<strong>de</strong>nt Information,<br />

Relations and Insertions in Bible<br />

As it is known, the transcen<strong>de</strong>nt mathematical numbers have the properties: a) do<br />

not <strong>de</strong>pend on any human artifacts (a true collection <strong>of</strong> remarkably mislea<strong>din</strong>g<br />

numerical artifacts is presented insi<strong>de</strong> the book: M. Gardner ”The magic numbers<br />

<strong>of</strong> dr. Matrix”, Prometheus Books, Buffalo, New York, 1985), as the numeration<br />

system, choice <strong>of</strong> numerical figures, personal data, etc., b) are unique for a given<br />

mathematical property, c) are irrational. We will <strong>de</strong>fine here the transcen<strong>de</strong>nt<br />

integers as the natural numbers which fulfil the first 2 [a) and b)] requirements.<br />

Examples <strong>of</strong> transcen<strong>de</strong>nt integers in Bible: (i) 153 (John 21:11) <strong>de</strong>fined as the<br />

unique solution M <strong>of</strong> the equations system in integer numbers:<br />

m<br />

i1<br />

n<br />

M i<br />

j!,<br />

(ii) 276 (Acts 27:37) – unique solution N <strong>of</strong> the equations system:<br />

j1<br />

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118 Dan Alexandru Iordache<br />

p<br />

N i<br />

j<br />

i1<br />

q<br />

j1<br />

5<br />

. Of course, the accurate quantitative explanation <strong>of</strong> the pointed<br />

out transcen<strong>de</strong>nt integers requires a rather difficult 1 additional study.<br />

The most important possible (or even probable) transcen<strong>de</strong>nt information<br />

elements in Bible refer to the cosmological predictions; some examples:<br />

a) Genesis 1:3 ”And God said: Let there be light, and there was light”; Genesis<br />

1:14 ”And God said: Let there be lights in the expanse <strong>of</strong> the sky to separate the<br />

day from the night …”, hence the light appeared before the stars, agreeing with<br />

the present «Big Bang» theory, which has found that the light appeared – through<br />

the photons escape from atoms (fig. 9) – much earlier than the stars;<br />

b) 2 Peter 3:8 ”With the Lord a day is like a thousand years, and a thousand years<br />

are like a day” - particular statement <strong>of</strong> the Special Theory <strong>of</strong> Relativity (see also<br />

Psalm 90:4);<br />

c) Hebrews 11:3 ”… what is seen was not ma<strong>de</strong> out <strong>of</strong> what was visible” -<br />

appearance <strong>of</strong> matter, space and time from nothing known, during the ”Big Bang”<br />

process;<br />

d) Job 9:8 ”He alone stretches out the heavens”; Isaiah 40:22 ”He stretches out<br />

the heavens like a canopy, and spreads them out like a tent to live in”; Isaiah 42:5<br />

”He who created the heavens and stretched them out” - the Universe expansion.<br />

Example <strong>of</strong> possible transcen<strong>de</strong>nt relations:<br />

It is known that insi<strong>de</strong> the extremely complex Bible structure are embed<strong>de</strong>d some<br />

amazing information (see e.g. [23] for the Old Testament). This work brings a<br />

new example <strong>of</strong> possible transcen<strong>de</strong>nt relation embed<strong>de</strong>d in Bible.<br />

Consi<strong>de</strong>r the 20 th century when the humankind succee<strong>de</strong>d [24] to evaluate the<br />

Universe age. Then (20 th century), the Genesis 7 th yowm [the Hebrew word yowm<br />

may be translated both by day (usually) or age/epoch] duration (accor<strong>din</strong>g to<br />

1 We will mention that many problems in the field <strong>of</strong> Numbers Theory are extremely difficult. E.g.,<br />

the statement <strong>of</strong> the (Pierre <strong>de</strong>) Fermat’s last (greatest) theorem was published in 1670 [20], by<br />

his el<strong>de</strong>st son – Clément Samuel Fermat, but its solution was found only in 1995 [21] by the<br />

American pr<strong>of</strong>essor Andrew Wiles. Wiles <strong>de</strong>scribes ([22], p. 236) his experience <strong>of</strong> doing<br />

mathematics in terms <strong>of</strong> a journey through a dark unexplored mansion: “One enters the first room<br />

<strong>of</strong> the mansion and it’s dark. Completely dark. One stumbles around bumping into the furniture,<br />

but gradually you learn where each piece <strong>of</strong> furniture is. Finally, after six months or so, you find<br />

the light switch, you turn it on, and sud<strong>de</strong>nly it’s all illuminated. You can see exactly where you<br />

were. Then you move in the next room and spend another six months in the dark. So each <strong>of</strong> these<br />

breakthroughs, while sometimes they’re momentary, sometimes over a period <strong>of</strong> one day or two,<br />

they are the culmination <strong>of</strong>, and couldn’t exist without, the many months <strong>of</strong> stumbling around in<br />

the dark that prece<strong>de</strong> them”.<br />

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Universe versus Multiverse 119<br />

Christian chronologies, as the Archbishop Ussher’s one [25]) is between 6000 and<br />

7000 years (indicated by God). Multiplying this duration with:<br />

a) 365.25 (number <strong>of</strong> days/year),<br />

b) then with 10 3 Earth years/God day (2 Peter 3:8), and finally:<br />

c) with 7 yowm in Genesis (2:2),<br />

one finds: 60007000 years indicated by God 365.2510 3 Earth years/God day<br />

7 Genesis yowm = (15.3417.9)10 9 Earth years, hence exactly the presently<br />

evaluated Universe age! Is this calculation a transcen<strong>de</strong>nt one? Yes! Is it<br />

meaningful? To answer it is necessary to know if its insertion in the Bible<br />

structure was transcen<strong>de</strong>nt, and … we do not know!<br />

This answer is valid also for the ”beast” number 666. It is obvious that this<br />

number is not transcen<strong>de</strong>nt (being significant in the <strong>de</strong>cimal numeration system),<br />

but … if it could have a transcen<strong>de</strong>nt insertion, it would have the role to represent<br />

numerically the false being - main humankind enemy (Satan).<br />

Conclusions<br />

It is well-known that at the beginning <strong>of</strong> the 20 th century, the Physics Nobel prizes<br />

were awar<strong>de</strong>d only to works experimentally confirmed; e.g. the absolutely<br />

outstan<strong>din</strong>g physicist Albert Einstein received (in 1921) the Physics Nobel prize<br />

for the theory <strong>of</strong> photoelectric effect (experimentally checked up) and not for his<br />

Special and General Relativity theories, which were still consi<strong>de</strong>red as<br />

insufficiently proven. Later, the successes <strong>of</strong> the theoretical Physics were so<br />

striking that in 1979 the theoreticians S.L. Glashow, A. Salam and S. Weinberg<br />

were awar<strong>de</strong>d by the Physics Nobel prize for their theory <strong>of</strong> unified weak and<br />

<br />

electromagnetic interaction, though the intermediary vector bosons W and Z 0<br />

predicted by them were not still discovered (they were experimentally found by<br />

C. Rubbia and S. van <strong>de</strong>r Meer only 4 years later). For such reasons, the<br />

confi<strong>de</strong>nce <strong>of</strong> physicists in the unified theories was so high that it was a <strong>de</strong>ep<br />

disappointment [17], [26] to find that these unified theories are not valid for the<br />

Universe evolution <strong>de</strong>scriptions.<br />

Taking into account that:<br />

a) while the masses <strong>of</strong> the intermediary vector bosons predicted by the unified<br />

theory <strong>of</strong> weak and electromagnetic interactions are only 2 magnitu<strong>de</strong> or<strong>de</strong>rs<br />

larger than that <strong>of</strong> protons,<br />

b) the parameters <strong>of</strong> the Big Bang processes are more than 25 magnitu<strong>de</strong> or<strong>de</strong>rs<br />

distant to somewhat « usual » ones, c) the Physics advance from Democrit’s<br />

atomistic theory to the quantum atomic Physics (over 7 magnitu<strong>de</strong> or<strong>de</strong>rs) require<br />

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120 Dan Alexandru Iordache<br />

more than 20 centuries, we don’t have to be exaggerate: even if now the Physics<br />

progresses are much accelerated, its advance over more than 25 magnitu<strong>de</strong> or<strong>de</strong>rs<br />

(up to the Big Bang field) will require probably several <strong>de</strong>ca<strong>de</strong>s (perhaps even<br />

centuries)! We have to be patient to be accumulated in the following <strong>de</strong>ca<strong>de</strong>s and<br />

(probably) centuries sufficient experimental data to be able to formulate valid<br />

theoretical cosmological mo<strong>de</strong>ls.<br />

As it concerns the Bible, it seems that: a) insi<strong>de</strong> the Bible structure are ”hid<strong>de</strong>n”<br />

some important information, b) the mo<strong>de</strong>rn Physics and the Bible predictions are<br />

convergent. That is why the Bible <strong>de</strong>serves a thorough study, for its scientific<br />

information, and not only for its outstan<strong>din</strong>g ethics recommendations (cultivate<br />

empathy, fight our selfishness, etc.). Despite the main goal <strong>of</strong> Bible is to improve<br />

the human beings ethical behaviour, it involves also some (rather few) scientific<br />

elements. However, one finds that the number <strong>of</strong> Bible sentences initially without<br />

any scientific meaning that got in the last centuries such a connotation is<br />

monotonically increasing, and even in an accelerated manner [e.g. (few examples)<br />

from the: a) transcen<strong>de</strong>nt integers (John 21:11, Acts 27:37) to the: b) role <strong>of</strong><br />

Information in the ”buil<strong>din</strong>g” <strong>of</strong> complex systems (Genesis 1:3), c) appearance<br />

or<strong>de</strong>r <strong>of</strong> light sources (Genesis 1:3 and 1:14), d) chromosomes (Genesis 2:22), d)<br />

ADN <strong>de</strong>fects and repairs, implicitly (Genesis 4 and 5), e) the special relativity<br />

theory (2 Peter 3:8), f) main features <strong>of</strong> the Big Bang process (see above), etc.].<br />

Either it happened that – between a tremendous number <strong>of</strong> parallel Universes,<br />

with different features [19a] – our Universe be the unique (acci<strong>de</strong>ntal) one [26]<br />

with suitable conditions for the life existence and (on Earth) <strong>of</strong> the intelligent life<br />

presence, or this Universe and Earth were created by supernatural <strong>de</strong>sign, it results<br />

that the humankind has a huge responsibility – to run optimally the only one<br />

World experiment, whose main actors we are.<br />

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Universe versus Multiverse 121<br />

R E F E R E N C E S<br />

1. a) DOBRESCU R., IORDACHE D., eds, Complexity Mo<strong>de</strong>lling (in Romanian), Politehnica<br />

Press Printing House, Bucharest, 2007; b) DOBRESCU R., IORDACHE D., Complexity and<br />

Information, Romanian Aca<strong>de</strong>my Printing House, 2010.<br />

2. IORDACHE D., Main complexity features <strong>of</strong> the thermo-mechanical evolution <strong>of</strong> the universe,<br />

chap. 5 in Research Trends in Mechanics, vol. 2, Romanian Aca<strong>de</strong>my Printing House, 2008.<br />

3. HARTLEY R.V.L., Transmission <strong>of</strong> Information, Bell System Techn. J., July 1928.<br />

4. a) SHANNON C., The Mathematical Theory <strong>of</strong> Communication, Bell Syst. Techn. J., 27, 379-<br />

423, 623-56(1948); ibid., 30, 50(1951); b) SHANNON C. E., WEAVER W., The mathematical<br />

theory <strong>of</strong> communications, Illinois Urbana Univ. Press, 1949.<br />

5. a) KHINCHIN A.J., Mathematical Foundations <strong>of</strong> Information Theory, Dover, New York,<br />

1957; b) KHINCHIN A.J., in Arbeiten zur Informationstheorie I, VEB Verlag, Berlin, 1961, pp. 7-<br />

85; c) KOLMOGOROV A.N., ibid., pp. 91-116; d) GUIAŞU S., Information theory with<br />

applications, McGraw Hill, New York, 1977.<br />

6. a) ANDERSON P.W., Science, 177, 293(1972); b) ANDERSON P.W., Proc. Natl. Acad.<br />

Science (USA), 92, 6653-6654(1995).<br />

7. a) SOLOMON S., SHIR E., Europhysics News, 34(2) 54-57(2003); b) SOLOMON S., Annual<br />

Reviews <strong>of</strong> Comp. Physics II, 243-294, D. Stauffer ed., World Scientific, 1995.<br />

8. a) GUKHMAN A. A., Introduction to the Theory <strong>of</strong> Similarity, Aca<strong>de</strong>mic Press, New York,<br />

1965; b) BARENBLATT G. I., Dimensional Analysis, Gordon and Breach, New York, 1987; c)<br />

BARENBLATT G. I., Scaling, Self-Similarity and Intermediate Asymptotics, Cambridge Texts in<br />

Applied Mathematics, 1996.<br />

9. BODEGOM E., IORDACHE D., Physics for Engineering Stu<strong>de</strong>nts, vol. 1, Classical Physics,<br />

Politehnica Press, Bucharest, 2007<br />

10. IORDACHE D., Contributions to the Study <strong>of</strong> Numerical Phenomena intervening in the<br />

Computer Simulations <strong>of</strong> some Physical Processes, Credis Printing House, Bucharest, 2004.<br />

11. DIRAC P.A.M., The Cosmological Constants, Nature 139, 323(1937).<br />

12. REES M., Just Six Numbers, Basic Books, 2000.<br />

13. DICKE R.H., Dirac’s Cosmology and Mach’s Principle, Nature 192, 440-441(1961).<br />

14. a) ROOD R.T., TREFIL J.S., Are we alone? The possibility <strong>of</strong> Extraterrestrial Civilisations,<br />

Scribner’s sons, New York, 1986; b) TIPLER F.J., The search for extraterrestrial life: recent<br />

<strong>de</strong>velopments, Physics Today, 40, 92, December 1987.<br />

15. WHEELER J.A., Foreword, in The Anthropic Cosmological Principle, Oxford, Clarendon<br />

Press, UK, 1986.<br />

16. EVERETT H., Many-World Interpretation <strong>of</strong> Quantum Mechanics, PhD Dissertation at<br />

Princeton, 1956.<br />

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122 Dan Alexandru Iordache<br />

17. SMOLIN L.: a) The Trouble with Physics, Houghton Mifflin Harcourt, 2006; b) Thread-Bar<br />

theories, IEEE Spectrum, January 2007, www.Spectrum.ieee.org/geek-life/tools-toys/ threadbartheories.0<br />

18. a) GUTH A. H., Inflationary Universe: A possible solution to the Horizon and Flatness<br />

problems, Physical Review D, 23, pp. 347-356(1981); b) GUTH A. H., STEINHARDT P. J., The<br />

Inflationary Universe, Scientific American, p. 116, May 1984; c) GUTH A. H., The inflationary<br />

universe. The quest for a new <strong>of</strong> cosmic origins, Addison-Wesley, Rea<strong>din</strong>g, 1997.<br />

19. a) LINDE A., The Self-Reproducing Inflationary Universe, Scientific American, pp. 48-55,<br />

November 1994; b) LINDE A., Particle physics and Inflationary cosmology, Physics Today, 40(9)<br />

61-68 (Sept. 1987), & treatise, Harwood Aca<strong>de</strong>mic Publishers, 1990; c) LINDE A., Inflation and<br />

Quantum cosmology, Aca<strong>de</strong>mic Press, 1990.<br />

20. FERMAT C.S., Diophantus’ Arithmetica containing (48) observations by P. <strong>de</strong> Fermat,<br />

Toulouse, 1670.<br />

21. A. WILES A., Modular elliptic curves and Fermat’s last theorem, Annals <strong>of</strong> Mathematics,<br />

142, 443-551(1995).<br />

22. SINGH S., Fermat’s Enigma: the Epic Quest to Solve the World’s Greatest Mathematical<br />

Problem, Walker Publishing Company, New York, 1997.<br />

23. a) WITZTUM D., RIPS E., ROSENBERG Y., Equidistant letters sequences in Genesis,<br />

Statistical Science, 9(3) 429-438(1994); b) M. Drosnin, The Bible co<strong>de</strong>, World Media Inc., vol. 1<br />

(1997), vol. 2 (2002).<br />

24. HUBBLE E., A relation between the distance and radial velocity among extra-galactic<br />

nebulae, Proc. National Aca<strong>de</strong>my <strong>of</strong> Sciences, 15, pp. 168-173(1929).<br />

25. JOHNSON P., A History <strong>of</strong> Christianity, Athenaeum, New York, 1976, p. 413.<br />

26. LIGHTMAN A.P., The acci<strong>de</strong>ntal Universe: Science’s crisis <strong>of</strong> faith, Harper’s Magazine,<br />

December 2011; d) www.harpers.org/archive/2011/12/0083720<br />

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Annals <strong>of</strong> the Aca<strong>de</strong>my <strong>of</strong> Romanian Scientists<br />

Series on Science and Technology <strong>of</strong> Information<br />

ISSN 2066-8562 Volume 5, Number 1/2012 123<br />

CHAOS AND STABILIZATION<br />

OF<br />

SELF-REMISSION TUMOR SYSTEM<br />

BY<br />

SLIDING MODE<br />

M.R. JAFARI 1 , M.R. ZARRABI 1,2 , S. EFFATI 1,3<br />

Abstract. In this paper a pray-predator system that called self-remission tumor is<br />

consi<strong>de</strong>red, and a new approach in or<strong>de</strong>r to stabilizing the unstable equilibrium<br />

points <strong>of</strong> self-remission tumor system with sli<strong>din</strong>g mo<strong>de</strong> control is introduced.<br />

The stability analysis <strong>of</strong> the biologically feasible equilibrium points is presented by<br />

using the Lyapunov function.<br />

A Lyapunov function is supposed for <strong>de</strong>signing a sli<strong>din</strong>g surface (SS).<br />

Lyapunov function is constructed to establish the global asymptotic stability <strong>of</strong> the<br />

uninfected and infected steady states by <strong>de</strong>scribing sli<strong>din</strong>g surface (SS), after that<br />

by consi<strong>de</strong>ring the <strong>de</strong>rivation <strong>of</strong> SS as zero, someone can achieve the equivalent<br />

control that inbreed system stays on SS and tends to equilibrium point in infinite<br />

horizon.<br />

In addition, numerical examples are presented to illustrate the effectiveness <strong>of</strong> the<br />

proposed method.<br />

Keywords: Chaos, Tumor, Equivalent control, Sli<strong>din</strong>g surface<br />

1. Introduction<br />

Cancer is one <strong>of</strong> the greatest killers in the world and the control <strong>of</strong> tumor growth<br />

requires special attention [9].<br />

The mathematical mo<strong>de</strong>ling <strong>of</strong> cancer self-remission and tumor has been<br />

approached by a few numbers <strong>of</strong> researchers un<strong>de</strong>r using a variety <strong>of</strong> mo<strong>de</strong>ls over<br />

the past <strong>de</strong>ca<strong>de</strong>s [8, 9, 13, 18].<br />

Many authors have discussed the problem <strong>of</strong> the chaotic behavior and stability<br />

analysis <strong>of</strong> some biological mo<strong>de</strong>ls such as cancer and tumor mo<strong>de</strong>l, genital<br />

herpes epi<strong>de</strong>mic, stochastic lattice gas prey-predator mo<strong>de</strong>s [7, 8, 13] and many<br />

other mo<strong>de</strong>ls.<br />

1 Department <strong>of</strong> Applied Mathematics, Ferdowsi University <strong>of</strong> Mashhad (see above picture),<br />

Mashhad, Iran, (mreza.jafari26@gmail.com).<br />

2 (mo.za870@gmail.com).<br />

3 (s-effati@um.ac.ir).<br />

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