Volume 2 - LENR-CANR

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We conjecture that -bonded dideuterium [7] (essentially molecular D2) forms in the vacancies at more modest loadings. These are the active sites, which occur in the outer (micron-scale) region of the cathode. Dideuterium formation can be modeled using simple statistical mechanics given an estimate of the binding energy. Excitation transfer is then stimulated by phonon exchange with compressional phonon modes (the matrix element between D2 and 4 He couples predominantly to compressional phonon modes) that are highly excited. Phonon excitation in this picture is produced by the deuterium flux through the nearsurface of the cathode. Energy exchange occurs in the presence of high compressional optical phonon excitation in the case of assumed 4 He-compact D2 states (which at present seems to match experiment best). The simplified model described above consisting of two-sets of twolevel systems to account for the nuclear states, and a harmonic oscillator (augmented with loss) to model optical phonon modes, can be used to develop equations describing the associated coherent dynamics for the simulation model. As energy is produced, 4 He accumulates in the active sites. At first, this would be helpful as there would be more capacity for anomalous energy exchange, since in general there is little helium present initially. However, as more energy is produced, we expect helium to block active sites, since the diffusion of helium away from the active sites is very slow near room temperature. In the event that helium diffusion limits excess heat production, we would expect to see a strong temperature dependence associated with excess heat production (as has been reported in a number of experiments [8]). With an appropriate simulation model, we can model this effect, and compute the fraction of helium released into the gas. We have begun the development of the simulation model outlined above. The results obtained so far seem to be interesting, and we hope to compare our results with experiment in the coming months. Appendix Consider the enhancement of multi-quantum coherent energy exchange in a many-spin spinboson model augmented with loss. We take the Hamiltonian to be of the form ˆ ˆ S 2S ˆ ˆ ˆ ˆ Where the first term in the Hamiltonian describes the energy of the two-level systems, the second term describes the oscillator, the third term implements linear coupling, and the final term accounts for the loss added to the model. The model is discussed further in [9]. 583 z † x † H E 0aa V a a i E 2
Figure 3. Energy levels that contribute to indirect coupling between |M,n and |M+1,n-5 in the case of multi-quantum exchange involving 5 quanta. The impact of loss on energy exchange can be illustrated through a concrete example. We consider a finite basis solution constructed from a combination of 12 basis states composed individually of products of Dicke states and oscillator states c S, M n j j j j We consider indirect coupling from an initial state |M,n to a final state |M+1,n-5, in which a single two-level system excitation is matched to a loss of 5 oscillator quanta. The states are illustrated in Figure 3. If no loss is present, the indirect matrix element between the initial state and the final state can be found to lowest-order in perturbation theory to be 5 625 V V1,12 n n 1 4 n 4 S M S M 1 0 64 E If loss is present and large for all intermediate states with a basis energy less than E, such that the associated paths do not contribute, then the indirect coupling matrix element is 1 4 3 2 2 V1,12 1,125 S 10S S 10M 8M 22 V 0 18 584
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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
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: of the weak coupling matrix element
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.,
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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
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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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