Volume 2 - LENR-CANR

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needs of an engineering project. Their scientific limitations are discussed by Norman Cook in his book, Models of Nuclear Physics, Springer 2006. Cook’s book and presentation at ICCF-14 provide a useful context for gaining a deeper understanding the history of development of the Fleischmann-Pons Effect and why it was controversial. We hope that, when finished, this Country History project will offer a better appreciation of what will be required to deal with some of the most fundamental problems of the physical sciences. 1. “Condensed Matter Nuclear Science” Research in China Presentation Title: Normal Temperature Nuclear Fusion Xing Z. Li, Department of Physics, Tsinghua University, Beijing Presentation at ICCF-14, Washington D.C., Aug.13 2008, Abstract. Five features of “Condensed Matter Nuclear Science” research in China are addressed. Five important meetings are described from the beginning to April of 2008. Twenty institutions are listed with their principle investigators, research staffs, and main research subjects. Twenty-nine articles are cited for reference. Nomenclature. Cold fusion is referred to as “normal temperature nuclear fusion” in China. It was given this name by Academician, Qian Xue Sen. In 2002, during ICCF-9, International Advisory Committee decided on a new name, Condensed Matter Nuclear Science (CMNS), in order to show the progress of the normal temperature nuclear fusion which had initiated this research field. This article mainly discusses the history; hence, it still adopts the name of normal temperature nuclear fusion (or in some cases “cold fusion”). Introduction. Normal temperature nuclear fusion has been conducted for 19 years in China. When reviewing it, five aspects of the research stand out: 1. National policy has always kept an expectation established at the beginning. 2. A group of top scientists have continued to support this research, even though it appears to violate common-sense. 3. International collaboration has been an important aspect from beginning until the present day. 4. Chinese researchers have attempted to develop the basic research independently with our own approaches. 5. Hot fusion institutions have kept abreast of development in normal temperature nuclear fusion, and have even given a hand occasionally. Over 20 institutions have continued research into these phenomena since the 1989 FPE announcement. The map below provides an indication of the work as of August 2008. 781
2. “Condensed Matter Nuclear Science” Research in France History of Cold Fusion France Jean-Paul Biberian, Faculté des Sciences de Luminy, Marseille Jacques Dufour, CNAM, Paris The players. These scientists and engineers have entered the field at one time or another : The CEA Grenoble (Georges Lonchampt). CNAM (Jacques Dufour). CNAM (Pierre Clauzon). The EDF (Electricité de France). Université Aix-Marseille (Jean-Paul Biberian). IMRA Sophia Antipolis (Stan Pons and Martin Fleischman). Independent researcher (Jean-Louis Naudin). Independent researcher (Fabrice David). Fondation Louis de Broglie (Georges Lochak and Henri Lehn). The future. Unless something striking happens soon, the field will disappear in France. Today’s active researchers” CNAM (Pierre Clauzon, already retired). Université Aix-Marseille (Jean-Paul Biberian, will retire in three years). Fondation Louis de Broglie(George Lochak and Henri Lehn, already retired). Fabrice David. 782
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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
Page 281 and 282: 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
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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
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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: Cold Fusion Country History Project
Page 335 and 336: need for a coordinated effort in ma
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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