Volume 2 - LENR-CANR

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Research interest among younger scientist can be found at CNAM where Jacques Dufour has a team of two young scientists actively testing a novel working hypothesis (picochemistry) that based on a current center of interest in main stream physics (long range weak Yukawa potential in the Standard Model Extension). 3. “Condensed Matter Nuclear Science” Research in India History of Cold Fusion Research in India M. Srinivasan, Formerly of Bhaba Atomic Research Centre, Trombay, Mumbai Phases of CF Research in India Phase i : 1989 to 1991 (ICCF 1) - Most productive era! Phase ii : 1992 to 1995 (ICCF 3,4,5) - Post Iyengar period Phase iii : 1996 to 2007 (12 years) India totally blanked out! Phase iv : 2008 Revival - Following NIAS meeting of 9th January 2008 Overview of BARC (1989-90) BARC has > 50 Divisions & 3000 Scientists! 12 teams (~ 50 scientists) took up challenge To verify “nuclear origin” of phenomenon Looked for neutrons & Tritium First neutrons detected on 21st April 1989! Within a year all teams reported both n & T Among first groups to find branching ratio anomaly namely (n/T) = ~ 1E (-7) ICENES Karlsruhe 4th to 7th July 1989 Report BARC 1500 (Aug ‘89) (Historical role!) ICCF 1 & Fusion Technology paper of Aug ‘90 with 50 authors summarize work of 89- 90! 4. “Condensed Matter Nuclear Science” Research in Italy Cold Fusion in Italy Francesco Scaramuzzi , LNF/INFN, Frascati – Italy Introduction. I will discuss a book produced by ENEA: “The history of Cold Fusion in Italy”. I will touch the following issues: - The book - The beginning of the Italian History of CF - The years of maximum effort - The decay - Comments Comments. - cold fusion is a reality - it is prominently a scientific problem, very much interesting at that 783
need for a coordinated effort in material science - it is important to convince the scientific world of the validity of the issue, through neat, reproducible experiments - it is still too early to put the accent on the possible applicative fall-outs, even though everyone hopes in them, in particular in the field of energy production. 5. “Condensed Matter Nuclear Science” Research in Japan Country History of Japanese Work on Cold Fusion - Toward further development of Condensed Matter Nuclear Science J. Kasagi Laboratory of Nuclear Science, Tohoku University Y. Iwamura Advanced Technology Research Center, MHI Abstract. We briefly summarize the history of Japanese work on cold fusion after 1989. Since the excellent work performed by Prof. Arata are introduced and discussed in the special session, we try to summarize other works in Japan. The history can be divided into three periods: the 1st period is from the announcement by Fleischmann and Pons to the ICCF3 Nagoya Conference (1989 - 1993); the 2nd period is during the New Hydrogen Energy (NHE) Project (1994 – 1998); and the 3rd after the NHE project (1999 – present). Characteristics of each period and the present situation are presented. Introduction. In the 19 years following the announcement of Professors Martin Fleischmann and Stanley Pons, much work on the cold fusion has been carried out in Japan as well as in other countries. The organizers of this conference have asked us to edit a document on “cold fusion” research in Japan. Many official reports for various projects, proceedings of domestic meetings on cold fusion and research papers describe the progress of this research in Japan. Thus, we thought that it is worthwhile to collect and summarize such records as an interim report in the cold fusion research. Since the excellent works performed by Prof. Arata were introduced and fully discussed in the special session of ICCF14, we have tried to summarize other work based on many official reports in Japan. The history of cold fusion research in Japan can be divided into three periods: the 1st period is from the announcement of F-P to the ICCF3 Nagoya Conference (1989 - 1993), the 2nd period is during the New Hydrogen Energy (NHE) Project (1994 – 1998), and the 3rd after the NHE project (1999 – present), as schematically shown in Fig. 1. We will show background and characteristics of each period, as well as notable research. 6. “Condensed Matter Nuclear Science” Research in Russia (Former Soviet Union) Status of Russian Research on Low Energy Nuclear Reactions in Non-Equilibrium Condensed Matter, Based on Publications in Peer-Reviewed Journals 784
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Proceedings of the 14th Internation
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Table of Contents VOLUME 1 Preface
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Photon Measurements 326 Excess Heat
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Investigation of Deuteron-Deuteron
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Introduction to Cavitation Experime
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Bubble Driven Fusion Roger Stringha
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to the density of muon fusion syste
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4.184 Joules/calorie to give Qo. No
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References 1. M. P. Brenner, S. Hil
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Experiments on stimulation of cavit
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foil (thickness 0.1 mm) was situate
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the external surface of thick wall
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Introduction to Materials The outco
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the foils, and the effects of subse
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Material Science on Pd-D System to
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level required higher current compa
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morphology, and surface morphology
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Figure 11. Evolution of the input a
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Electrode Surface Morphology Charac
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fundamental peak; on the other hand
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RPSD@ max (x10 -32 m 4 ) 0.20 0.10
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2. V. Violante, F. Sarto, E.Castagn
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Experimental Starting with the meta
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Figure 3.1. A typical database reco
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palladium lot as received. Differen
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Condensed Matter “Cluster” Reac
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Loading Measurements A high-vacuum
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Reaction Rate Estimates An estimate
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References 1. Andrei Lipson, Brent
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Introduction to the Theory Papers P
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Foundations: Experimental Evidence,
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Such results are applicable to a wi
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electrostatic fields, that could ge
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Theory Papers 1. V. Adamenko & V.I.
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Figure 1. The general view and deta
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So with a high probability the unkn
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Potential energy of pair (without m
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the corresponding electron wave fun
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applicable in case of interaction o
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The expression in the exponent of (
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Empirical System Identification (ES
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esults of the previous sections to
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The higher the mass of a particle (
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The Hubbard model [18, 19], along w
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A B Figure 2. Atomic Arrangements o
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deuterons, their interaction is aff
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expected in D-D reactions is that w
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It is being argued that, while heav
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with odd permutations weighted by -
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20. C. Elsasser, K.M. Ho, C.T. Chan
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must have positive Bose Exchange sy
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these different statements that ref
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Fig.2 shows a pictorial representat
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(a) A Pictorial Representation of V
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esonance” can take place, in whic
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interior boundaries of the ordered
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Interface Model of Cold Fusion Talb
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D + Bloch "atom" sublayer, 3) epita
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sometimes stimulating an irreversib
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Toward an Explanation of Transmutat
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Given the well-established validity
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The next question is, therefore, if
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An Experimental Device to Test the
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Figure 1. Palladium/deuterium total
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Experimental Reaction enthalpies of
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10. J. Dufour, X. Dufour, D. Murat
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Together with the Coulomb-repulsion
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“The Coulomb Barrier not Static i
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2 16 2 gc 27 3 So, a solution for
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Moreover, we study the “nuclear e
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Then, according to the loading quan
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Having mapped that the -phase depen
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Considering the attractive force, d
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The expression (45) was partially e
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Table 1. Using the phase potential
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10. A.De Ninno et al. Europhysics L
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Fusion system still outperformed th
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Van der Waals attraction occurs at
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Quantum Fusion (QF) Quantum Fusion
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Energy exchange There is some exper
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of the weak coupling matrix element
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Figure 3. Energy levels that contri
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Input to Theory from Experiment in
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substrate, and excess heat is obser
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4. Laser stimulation Letts and Crav
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energetic particles are produced, o
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15. K. Kunimatsu, N. Hasegawa, A. K
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A Theoretical Formulation for Probl
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at some point we will require tools
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3. Matrix element example The appro
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Now the wavefunction on the RHS has
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Theory of Low-Energy Deuterium Fusi
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If mobile deuterons in a metal are
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allowed since [Z1/m1] = [Z2/m2], an
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traps (in 3g of Pd particles with a
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9. S.N. Bose, Z. Phys. 26, 178 (192
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system composed of host nuclei and
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A simple specific form of beff (p)
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Nuclear Transmutations in Polyethyl
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Furthermore, there are interesting
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The NT’s in phenanthrene [7] may
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explains why there is no neutron em
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T+T Fusion CrossSection (Barn) T+T
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science, the incident energy is so
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When the incident energy approaches
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9. Chadwick, M. B., Oblozinsky, P.,
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He = Em C + m Cm + tmn (C + m Cm
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where k 2 = (2 Md Ea / ħ ) = Md 2
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y altering the shape of the Coulomb
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Analysis and Confirmation of the
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This is the basic Langevin equation
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The fusion rate is calculated by th
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EQPET molecule must go back and con
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Introduction to Challenges and Summ
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notes that the common usage of the
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insufficient to allow us to reprodu
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in the early days of semiconductors
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Water In Acrylic Toppiece Gas Tube
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Much of this uncertainty would be r
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Figure 5. The effect of input power
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maximum values. From these values w
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considerably that they were enginee
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Technogies”, in 11th Internationa
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Self-Polarisation of Fusion Diodes:
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We propose that in this field of on
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Results A. Self-sustained voltage O
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Figure 6. Differential calorimeter
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Weight of Evidence for the Fleischm
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Figure 1. Multiple support for a hy
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P(D | T) = P(T | D) P(D) / P(T) = 0
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For more information about Bayesian
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positive is in the range 0.980 ± 0
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With the notation Emn = “m heads
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3.1. Selected papers Cravens and Le
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Table 3. P(Eif | Pf) Table 4. P(Ein
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Condensed Matter Nuclear Science”
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4. J. Breese and D. Koller, “Tuto
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Taking the nuclear origin of copiou
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The evolution of protoscience into
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References 1. Mosier-Boss, P.A., et
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Cold fusion (CF) is a potentially r
Page 283 and 284: ISCMNS has initiated a CF-dedicated
Page 285 and 286: Table 2. Current Methods and Propos
Page 287 and 288: For the CF/OSSc project, the ISCMNS
Page 289 and 290: ole of skeptical mainstream physici
Page 291 and 292: sized Pd and Pd alloy particles. Ap
Page 293 and 294: Honoring Pioneers For most fields o
Page 295 and 296: A&Z introduced new terms to describ
Page 297 and 298: The top portion of Fig. 3 shows plo
Page 299 and 300: Figure 7. New catalyst shows nano-P
Page 301 and 302: catalyst to outer vessel wall is 7
Page 303 and 304: Establishment of the “Solid Fusio
Page 305 and 306: Figure 1. Experimental Device Figur
Page 307 and 308: [The protocol for producing the ZrO
Page 309 and 310: Figure 5A. Comparison of generation
Page 311 and 312: Figure 6. Gas pressure characterist
Page 313 and 314: Note on Sources The Abstract is a r
Page 315 and 316: 37. Arata Y, Zhang Y-C; Proc. Japan
Page 317 and 318: LENR Research using Co-Deposition S
Page 319 and 320: that the tritium production was spo
Page 321 and 322: (a) (b) (c) Figure 4. Images obtain
Page 323 and 324: SPAWAR Systems Center-Pacific Pd:D
Page 325 and 326: 7. S. Szpak, P.A. Mosier-Boss, S.R.
Page 327 and 328: 17. S. Szpak, P.A. Mosier-Boss, and
Page 329 and 330: Preparata Prize Acceptance Speech I
Page 331 and 332: Cold Fusion Country History Project
Page 333: 2. “Condensed Matter Nuclear Scie
Page 337 and 338: Colloid J. USSR 48, 8(1986)). In 19
Page 339 and 340: scientists on the problem of Cold F
Page 341 and 342: Financial support for the conferenc
Page 343 and 344: Author Index Pages are in Volume 1
Page 345: Wang, J., 299 Watanabe, A., 338 Wei
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