Volume 2 - LENR-CANR

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Figure 1. Comparison of cluster trapping potential between 4D/TSC and 6D 2- /OSC. TSC condenses ultimately to very small Rdd value (ends at Rdd-min=about 20 fm), while OSC converges at Rdd=about 40 pm (corresponding to the ground state). Figure 2. Numerical solution of Eq. (2) by the Verlet method 3) . Time is reversed starting from the condensation time 1.4007 fs. 665
The fusion rate is calculated by the following Fermi’s golden rule 3,4,6) , nd 2 W 21 Pnd ( r0 ) 3. 04 10 Pnd ( r0 ) W (4) Here Pnd is barrier factor for nD-cluster and is the averaged value of imaginary part of nuclear optical potential 3,4) . The extrapolation of value to 4d fusion was made 3) by using the scaling law W 5 ( PEF ) with PEF-value which is given in unit of derivative of one pion exchange potential (OPEP) (a simple case of Hamada-Johnston potential 4) for the pion exchange model). We estimated the next value of 4D fusion yield per TSC generation, t c 1 exp( ( t ) dt ) (5) 4 d 0 4 d Using time-dependent barrier factors, we obtained 3) 4 1. 0 d . This result means that we have obtained a simple result that 4D fusion may take place with almost 100% yield per TSC generation, so that macroscopic 4d fusion yield is given simply with TSC generation rate Qtsc in the experimental conditions of CMNS. The ultimate condensation is possible only when the double Platonic symmetry of 4D/TSC is kept in its dynamic motion. The sufficient increase (super screening) of barrier factor is also only possible as long as the Platonic symmetric 4D/TSC system is kept. Therefore, there should be always 4 deuterons in barrier penetration and fusion process, so that 4d simultaneous fusion should take place predominantly. The portion of 2D (usual) fusion rate is considered to be negligible 3) . The order (or constraint) of condensed matter incubates this 6) . Typical nuclear products of 4D fusion are predicted to be two 23.8 MeV α-particles, although the final state interaction of 8 Be* is complex, and yet to be studied 5,6) . 3. Time Dependent QM Behavior of Electron Clouds We consider now the principle of dynamic condensation motion of TSC in the view of Heisenberg uncertainty principle (HUP). At the starting condition of 4D/TSC (t=0), d-d distance Rdd was estimated to be the same value (74.1 pm) as that of a D2 molecule. At this starting point, the mean electron kinetic energy of one “d-e-d-e” face EQPET molecule out of TSC 6 faces was 17.6 eV (19 eV by semi-classical model 6) ). During the non-linear condensation of TSC, the size of “d-e-d-e” EQPET molecule as a face of 4D/TSC decreases from Rdd=74.1 pm at t=0 to Rdd=20.6 fm at t=1.4007 fs. In the view of HUP, electron wave length should decrease accordingly to the decrement of Rdd. At around t=1.4007 fs, the mean kinetic energy of electron for “d-e-d-e” EQPET molecule was estimated 3) to be 57.6 keV. The original Langevin equation for D2 molecule, before the quantum-mechanical ensemble averaging is done, as given by, 2 2 2 d Rdd e 2meve Vs2 ( Rdd ; 1, 1) md ( 4 2 2) f ( t) (6) 2 2 dt Rdd ( Ree / 2) Rdd We consider the averaged force-balance between the first term and the second term of right side of Eq. (6), with ensemble averaging by weight of “adiabatic electron wave function” of 666
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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
Page 171 and 172: energetic particles are produced, o
Page 173 and 174: 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: This is the basic Langevin equation
Page 225 and 226: EQPET molecule must go back and con
Page 227 and 228: Introduction to Challenges and Summ
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”
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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
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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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