Volume 2 - LENR-CANR

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TSC, with a tail of time-varying effective wave length. This does not contradict the Heisenberg uncertainty principle. A more detailed paper on this work will appear in JCMNS 7) . References 1) A. Takahashi: A theoretical summary of condensed matter nuclear effects, J. Condensed Matter Nuclear Science, 1(2007)129-141 2) A. Takahashi, N. Yabuuchi: Condensed matter nuclear effects under Platonic symmetry, Proc. ICCF13, Sochi, Russia, 2007 (to be published) 3) A. Takahashi, N. Yabuuchi: Study on 4D/TSC condensation motion by non-liniear Langevin equation, LENR Source Book, American Chemical Society, 2007, to be published from Oxford Univ. Press, August 2008 4) A. Takahashi, N. Yabuuchi: D-cluster dynamics and fusion rate by Langevin equation, Proc. 8 th Int. Workshop on Anomalies in D/H Loaded Metals, Catania, Italy, 2007, to be published in 2008 5) A. Takahashi: A chronicle of condensed cluster fusion models, Proc. JCF8, Kyoto, 2007, pp.51-62, Japan CF Research Society, 2008 6) Akito Takahashi: “Cold Fusion 2008 – mechanism of condensed cluster fusion” (in Japanese), Kogakusha, Tokyo, 2008 7) Akito Takahashi: Dynamic Motion of TSC Condensation Motion, submitted to JCMNS, September 2008 669
Introduction to Challenges and Summary The field of LENR has all the challenges of any accepted part of science, plus the burden of gaining acceptance and recognition as a legitimate field of scientific inquiry. The normal challenges include the design and performance of sound experiments, and the development and application of theories to explain past observations or make predictions. They also include communications of results through discussions, presentations and journal articles. Now, all of these things do apply to LENR, although it is difficult or impossible to get many of the appropriate journals to even consider papers from scientists in the field. The problem of LENR becoming a recognized field of scientific research is very challenging. Acceptance as a part of science would have far reaching consequences. Now, in the US, responsible people in both the Congress and the Administration correctly assert that they are not scientists. They are waiting for the scientific community to examine LENR and pronounce judgment, not on its details, but only whether or not it should be considered as a science. Administrators in the US Patent and Trademark Office, who are not scientists, have the same refrain. They await scientists with relevant competencies to examine information on LENR and render an opinion on its being, or not being, part of science. Those responsible for documentation and communication of scientific results, the editors of scientific journals and magazines, also correctly assert note that they are not scientists (even though many of them were scientists earlier in their careers). They want others, who are now practicing (publishing) scientists, to examine results on LENR and say what they think about the field as a science. So, why is are key scientists individually and the scientific community, broadly considered, unwilling to (a) examine the evidence, (b) draw conclusions about the nature of work on LENR and (c) communicate them to other scientists and the public? Part of the reason is that most scientists are busy with their own research, and not willing to spend time on examining LENR information. There is, after all, little likelihood of either support or fame in such an activity. Some scientists are fear-filled as a result of the residual poor reputation of the field. They are afraid that their reputations would be tainted and, maybe, their careers destroyed. Then, there are a few very prominent and vocal ex-scientists who speak out against the field even though they seem not to be aware of key results from LENR research. They may have had strong scientific careers at one time, but they no longer contribute to the advancement of knowledge by actually doing research and publishing the results. Whatever motivates these people, money or ego or anything else, they do themselves and the field a real disservice. This is especially true in the case of LENR. It is uncertain if and when the current research phase of LENR will be the basis for practical energy sources. However, the prospects of small distributed nuclear power sources, without dangerous prompt radiation nor significant radioactive waste, deserves consideration. Those possibilities are in addition to the wonderful scientific challenge of understanding how it is possible to stimulate MeV nuclear reactions by using eV chemical energies. Whether or not LENR energy sources prove to be important, there are some basic requirements for the operation of LENR experiments. One of the most fundamental is replication. Hence, this conference included an invited paper by McKubre on replication. He 670
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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
Page 175 and 176: A Theoretical Formulation for Probl
Page 177 and 178: at some point we will require tools
Page 179 and 180: 3. Matrix element example The appro
Page 181 and 182: Now the wavefunction on the RHS has
Page 183 and 184: Theory of Low-Energy Deuterium Fusi
Page 185 and 186: If mobile deuterons in a metal are
Page 187 and 188: allowed since [Z1/m1] = [Z2/m2], an
Page 189 and 190: traps (in 3g of Pd particles with a
Page 191 and 192: 9. S.N. Bose, Z. Phys. 26, 178 (192
Page 193 and 194: system composed of host nuclei and
Page 195 and 196: A simple specific form of beff (p)
Page 197 and 198: Nuclear Transmutations in Polyethyl
Page 199 and 200: Furthermore, there are interesting
Page 201 and 202: The NT’s in phenanthrene [7] may
Page 203 and 204: explains why there is no neutron em
Page 205 and 206: T+T Fusion CrossSection (Barn) T+T
Page 207 and 208: science, the incident energy is so
Page 209 and 210: When the incident energy approaches
Page 211 and 212: 9. Chadwick, M. B., Oblozinsky, P.,
Page 213 and 214: He = Em C + m Cm + tmn (C + m Cm
Page 215 and 216: where k 2 = (2 Md Ea / ħ ) = Md 2
Page 217 and 218: y altering the shape of the Coulomb
Page 219 and 220: Analysis and Confirmation of the
Page 221 and 222: This is the basic Langevin equation
Page 223 and 224: The fusion rate is calculated by th
Page 225: EQPET molecule must go back and con
Page 229 and 230: notes that the common usage of the
Page 231 and 232: insufficient to allow us to reprodu
Page 233 and 234: in the early days of semiconductors
Page 235 and 236: Water In Acrylic Toppiece Gas Tube
Page 237 and 238: Much of this uncertainty would be r
Page 239 and 240: Figure 5. The effect of input power
Page 241 and 242: maximum values. From these values w
Page 243 and 244: considerably that they were enginee
Page 245 and 246: Technogies”, in 11th Internationa
Page 247 and 248: Self-Polarisation of Fusion Diodes:
Page 249 and 250: We propose that in this field of on
Page 251 and 252: Results A. Self-sustained voltage O
Page 253 and 254: Figure 6. Differential calorimeter
Page 255 and 256: Weight of Evidence for the Fleischm
Page 257 and 258: Figure 1. Multiple support for a hy
Page 259 and 260: P(D | T) = P(T | D) P(D) / P(T) = 0
Page 261 and 262: For more information about Bayesian
Page 263 and 264: positive is in the range 0.980 ± 0
Page 265 and 266: With the notation Emn = “m heads
Page 267 and 268: 3.1. Selected papers Cravens and Le
Page 269 and 270: Table 3. P(Eif | Pf) Table 4. P(Ein
Page 271 and 272: Condensed Matter Nuclear Science”
Page 273 and 274: 4. J. Breese and D. Koller, “Tuto
Page 275 and 276: 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
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ISCMNS has initiated a CF-dedicated
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Table 2. Current Methods and Propos
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For the CF/OSSc project, the ISCMNS
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ole of skeptical mainstream physici
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sized Pd and Pd alloy particles. Ap
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Honoring Pioneers For most fields o
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A&Z introduced new terms to describ
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The top portion of Fig. 3 shows plo
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Figure 7. New catalyst shows nano-P
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catalyst to outer vessel wall is 7
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Establishment of the “Solid Fusio
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Figure 1. Experimental Device Figur
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[The protocol for producing the ZrO
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Figure 5A. Comparison of generation
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Figure 6. Gas pressure characterist
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Note on Sources The Abstract is a r
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37. Arata Y, Zhang Y-C; Proc. Japan
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LENR Research using Co-Deposition S
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that the tritium production was spo
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(a) (b) (c) Figure 4. Images obtain
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SPAWAR Systems Center-Pacific Pd:D
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7. S. Szpak, P.A. Mosier-Boss, S.R.
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17. S. Szpak, P.A. Mosier-Boss, and
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Preparata Prize Acceptance Speech I
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Cold Fusion Country History Project
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2. “Condensed Matter Nuclear Scie
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need for a coordinated effort in ma
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Colloid J. USSR 48, 8(1986)). In 19
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scientists on the problem of Cold F
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Financial support for the conferenc
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Author Index Pages are in Volume 1
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Wang, J., 299 Watanabe, A., 338 Wei
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