Volume 2 - LENR-CANR

More documents

Recommendations

Info

capture of an electron by a deuteron, followed by decay of a triton.” This is written as p + d + e – → T + ν followed by T → 3 He + e – + , though “K-capture of an electron by a deuteron” would seem to hint at the transitory existence of a dineutron, 2 n, during the first reaction. This brings us to the paper by Peter Hagelstein and Irfan Chaudhary (12). Though screening is addressed, the main thrust of the paper is how a large quantum of energy, on the order of 24 MeV, can get distributed to the lattice as a very large number of quanta of vibrational modes, each on the order of a small fraction of an eV. The authors have studied models of a two-level system with a large transition energy (such as D2 and 4 He separated by 24 MeV) coupled to a low-energy harmonic oscillator, representing phonon modes. (These are reminiscent of multi-spin spin-boson models that occur in other contexts.) Because the coupling is weak due to the Gamow factor associated with the Coulomb barrier, they are led to consider (1) a loss term to suppress destructive interferences and (2) a second two-level system strongly coupled to the oscillator. Candidates for the second two-level system are discussed. This work is one part of a very ambitious program to model the FPE in detail from established basic principles. It takes place within a general framework described in the paper by Hagelstein et al. (14) already discussed above. Transmutation In previous work, V. Adamenko and V. I. Vysotskii (1) reported observations that suggested transmutations such as 27 Al + 12 C → 39 K in high-current electron-beam experiments. They hypothesized that such reactions were promoted by magnetic monopoles. In this paper, they make inferences about the properties of the monopoles and discuss possible mechanisms for their creation. The paper by Norman D. Cook (7) considers a lattice model of nuclear structure, an alternative to the usual shell, liquid-drop, cluster, and other models. The lattice model has previously been applied to explaining the asymmetric fission of uranium. It is applied here to observations of palladium cathodes by T. Mizuno suggesting transmutations of the form Pd + D → (fission products) for various isotopes of Pd. The “water tree” in the title of the paper by Hideo Kozima and Hiroshi Date (17) is a micron-scale defect, filled with electrolyte, which forms in polyethylene subjected to intense electric fields and has been implicated in failures of polyethylene-insulated power lines. The authors propose an explanation for observations by T. Kumazawa et al. that suggest various transmutations associated with the formation of water trees. The explanation is based on the authors’ “neutron-drop model,” developed in earlier work, which hypothesized the existence of a “dense neutron liquid at boundary / surface regions of . . . crystals” that contains “neutron drops,” denoted A ZΔ, having Z protons, Z electrons, and (A − Z) neutrons. The transmutations in question could be attributed to absorption by a nucleus of a neutron, with or without subsequent beta-decay, or to absorption of a 4 2Δ or an 8 4Δ. Finally, it should be noted that not all theoretical concepts for <strong>LENR</strong> were represented at ICCF-14. Hence this section, whilc relatively comprehensive, is necessarily incomplete. 482
Theory Papers 1. V. Adamenko & V.I. Vysotskii, The possible mechanism of creation of light magnetic monopoles in strong magnetic field of a laboratory system 2. D. Alexandrov, Heavy Electrons in Nano-Structure Clusters of Disordered Solids 3. R. W. Bass & M. Swartz, Empirical System Identification (ESID) and Optimal Control of Lattice-Assisted Nuclear Reactors 4. B.R. Breed, Can Established Physical Principles Explain Solid-State Fusion? 5. S.R. Chubb, Resonant Electromagnetic-Dynamics Explains the Fleischmann-Pons Effect 6. T.A. Chubb, Interface Model of Cold Fusion 7. N. Cook, Toward an Explanation of Transmutation Products on Palladium Cathodes 8. J. Dufour et al., An Experimental Device to Test the YPCP (“Yukawa Pico Chemistry and Physics”) Model: Implications for the CF-<strong>LENR</strong> Field 9. C. Fou, Investigation of Deuteron-Deuteron Cold Fusion in a Cavity 10. F. Frisone, “The Coulomb Barrier not Static in QED,” A correction to the Theory by Preparata on the Phenomenon of Cold Fusion and Theoretical hypothesis 11. R. Godes, Quantum Fusion Hypothesis 12. P.L. Hagelstein & I. Chaudhary, Excitation transfer and energy exchange processes for modeling the Fleischmann-Pons excess heat effect 13. P.L. Hagelstein, M.E. Melich, & R. Johnson, Input To Theory From Experiment In The Fleischmann-Pons Effect 14. P.L. Hagelstein et al., A Theoretical Formulation for Problems in Condensed Matter Nuclear Science 15. Y.E. Kim, Theory of Low-Energy Deuterium Fusion in Micro/Nano-Scale Metal Grains and Particles 16. H. Kozima, Complexity in the Cold Fusion Phenomenon 17. H. Kozima and H. Date, Nuclear Transmutations in Polyethylene (XLPE) Films and Water Tree Generation in Them 18. X.Z. Li et al., Exploring a Self-Sustaining Heater without Strong Nuclear Radiation 19. K.P. Sinha & A. Meulenberg, A model for enhanced fusion reaction in a solid matrix of metal deuterides 20. M. Swartz, Optimal Operating Point Manifolds in Active, Loaded Palladium Linked to Three Distinct Physical Regions 21. M. R. Swartz & L. P. G. Forsley, Analysis of “Superwave-as-Transitory-OOP-Peak” Hypothesis 22. Takahashi, Dynamic Mechanism of TSC Condensation Motion 483
Page 1 and 2:
Proceedings of the 14th Internation
Page 3 and 4:
Table of Contents VOLUME 1 Preface
Page 5 and 6:
Photon Measurements 326 Excess Heat
Page 7 and 8:
Investigation of Deuteron-Deuteron
Page 9 and 10:
Introduction to Cavitation Experime
Page 11 and 12:
Bubble Driven Fusion Roger Stringha
Page 13 and 14:
to the density of muon fusion syste
Page 15 and 16: 4.184 Joules/calorie to give Qo. No
Page 17 and 18: References 1. M. P. Brenner, S. Hil
Page 19 and 20: Experiments on stimulation of cavit
Page 21 and 22: foil (thickness 0.1 mm) was situate
Page 23 and 24: the external surface of thick wall
Page 25 and 26: Introduction to Materials The outco
Page 27 and 28: the foils, and the effects of subse
Page 29 and 30: Material Science on Pd-D System to
Page 31 and 32: level required higher current compa
Page 33 and 34: morphology, and surface morphology
Page 35 and 36: Figure 11. Evolution of the input a
Page 37 and 38: Electrode Surface Morphology Charac
Page 39 and 40: fundamental peak; on the other hand
Page 41 and 42: RPSD@ max (x10 -32 m 4 ) 0.20 0.10
Page 43 and 44: 2. V. Violante, F. Sarto, E.Castagn
Page 45 and 46: Experimental Starting with the meta
Page 47 and 48: Figure 3.1. A typical database reco
Page 49 and 50: palladium lot as received. Differen
Page 51 and 52: Condensed Matter “Cluster” Reac
Page 53 and 54: Loading Measurements A high-vacuum
Page 55 and 56: Reaction Rate Estimates An estimate
Page 57 and 58: References 1. Andrei Lipson, Brent
Page 59 and 60: Introduction to the Theory Papers P
Page 61 and 62: Foundations: Experimental Evidence,
Page 63 and 64: Such results are applicable to a wi
Page 65: electrostatic fields, that could ge
Page 69 and 70: Figure 1. The general view and deta
Page 71 and 72: So with a high probability the unkn
Page 73 and 74: Potential energy of pair (without m
Page 75 and 76: the corresponding electron wave fun
Page 77 and 78: applicable in case of interaction o
Page 79 and 80: The expression in the exponent of (
Page 81 and 82: Empirical System Identification (ES
Page 83 and 84: esults of the previous sections to
Page 85 and 86: The higher the mass of a particle (
Page 87 and 88: The Hubbard model [18, 19], along w
Page 89 and 90: A B Figure 2. Atomic Arrangements o
Page 91 and 92: deuterons, their interaction is aff
Page 93 and 94: expected in D-D reactions is that w
Page 95 and 96: It is being argued that, while heav
Page 97 and 98: with odd permutations weighted by -
Page 99 and 100: 20. C. Elsasser, K.M. Ho, C.T. Chan
Page 101 and 102: must have positive Bose Exchange sy
Page 103 and 104: these different statements that ref
Page 105 and 106: Fig.2 shows a pictorial representat
Page 107 and 108: (a) A Pictorial Representation of V
Page 109 and 110: esonance” can take place, in whic
Page 111 and 112: interior boundaries of the ordered
Page 113 and 114: Interface Model of Cold Fusion Talb
Page 115 and 116: D + Bloch "atom" sublayer, 3) epita
Page 117 and 118:
sometimes stimulating an irreversib
Page 119 and 120:
Toward an Explanation of Transmutat
Page 121 and 122:
Given the well-established validity
Page 123 and 124:
The next question is, therefore, if
Page 125 and 126:
An Experimental Device to Test the
Page 127 and 128:
Figure 1. Palladium/deuterium total
Page 129 and 130:
Experimental Reaction enthalpies of
Page 131 and 132:
10. J. Dufour, X. Dufour, D. Murat
Page 133 and 134:
Together with the Coulomb-repulsion
Page 135 and 136:
“The Coulomb Barrier not Static i
Page 137 and 138:
2 16 2 gc 27 3 So, a solution for
Page 139 and 140:
Moreover, we study the “nuclear e
Page 141 and 142:
Then, according to the loading quan
Page 143 and 144:
Having mapped that the -phase depen
Page 145 and 146:
Considering the attractive force, d
Page 147 and 148:
The expression (45) was partially e
Page 149 and 150:
Table 1. Using the phase potential
Page 151 and 152:
10. A.De Ninno et al. Europhysics L
Page 153 and 154:
Fusion system still outperformed th
Page 155 and 156:
Van der Waals attraction occurs at
Page 157 and 158:
Quantum Fusion (QF) Quantum Fusion
Page 159 and 160:
Energy exchange There is some exper
Page 161 and 162:
of the weak coupling matrix element
Page 163 and 164:
Figure 3. Energy levels that contri
Page 165 and 166:
Input to Theory from Experiment in
Page 167 and 168:
substrate, and excess heat is obser
Page 169 and 170:
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 and 222:
This is the basic Langevin equation
Page 223 and 224:
The fusion rate is calculated by th
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”
Page 273 and 274:
4. J. Breese and D. Koller, “Tuto
Page 275 and 276:
Taking the nuclear origin of copiou
Page 277 and 278:
The evolution of protoscience into
Page 279 and 280:
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
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 and 334:
2. “Condensed Matter Nuclear Scie
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
show all

Volume 2 - LENR-CANR

You also want an ePaper? Increase the reach of your titles

Delete template?

Save as template?