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eh - + p + → n + νl Where p + , n and νl designate proton, neutron and neutrino respectively. In order for this process to take place the following threshold condition about the effective mass of heavy electron eh - must be fulfilled [3]: 496 (12) β = meff / m0 > 2.531 (13) The effective masses from Table 1 even for strong field interactions (except for InxAl1-xN) fulfill the condition (13). It must be noted that certain particles must reach the region where the heavy electron is localized for the interaction to occur; i.e., the probability of the interaction of heavy electron– particle is higher in nano-layers or in nano-structure clusters that are close to the surface. Conclusion This paper can be considered the author’s first contribution in the field of interaction of charged particles with electrons localized in solids. Although the existence of heavy electrons in nano-structures is shown theoretically the author considers that the conditions about weak interaction in solids must be found in order further study of heavy electron-particle interactions to be performed. Finding of these conditions will be subject of a future work. Future work will also consider the role of heavy electrons in metallic hydride nano-layers. References 1. L. D. Landau, E. M. Lifshitz, The Classical Theory of Fields, Pergamon Press, Oxford (1975) 2. V. B. Berestetskii, E. M. Lifshitz, L. P. Pitaevskii, Quantum Electrodynamics, Butterworth Heinmann, Oxford (1997) 3. A. Widom, L. Larsen, Eur. Phys. Journal C, 46, 107 (2006) 4. P. L. Hagelstein, I. U. Chaudhary, Electron mass shift in nonthermal systems (D. Nagel, private communication) 5. D. Alexandrov, Journal of Crystal Growth, 246, 325 (2002) 6. D. Alexandrov, S. Butcher, M. Wintrebert-Fouquet, Journal of Vacuum Science and Technology, A22(3), 954 (2004) 7. D. Alexandrov, S. Butcher, T. Tansley, Physica Status Solidi, 203, 25 (2006) 8. D. Alexandrov, S. Butcher, T. Tansley, Journal of Crystal Growth, 288, 261 (2006) 9. A. S. Davydov, Quantum Mechanics, Pergamon Press, Oxford (1965) 10. K. F. Brennan, The Physics of Semiconductors, Cambridge University Press, Cambridge (1999) 11. R. E. Marshak, Riazuddin, C. P. Ryan, Theory of Weak Interaction of Elementary Particles, Interscience, New York (1969)
Empirical System Identification (ESID) and Optimal Control of Lattice-Assisted Nuclear Reactors Robert W. Bass 1 and Mitchell Swartz 2 1 Innoventek Inc. 2 JET Energy, Inc. Dr. Mitchell Swartz does not wish to have his papers uploaded to <strong>LENR</strong>-<strong>CANR</strong>.org. A copy of this paper can be found here: http://www.iscmns.org/iccf14/ProcICCF14b.pdf 497
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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
Page 7 and 8:
Investigation of Deuteron-Deuteron
Page 9 and 10:
Introduction to Cavitation Experime
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Bubble Driven Fusion Roger Stringha
Page 13 and 14:
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
Page 19 and 20:
Experiments on stimulation of cavit
Page 21 and 22:
foil (thickness 0.1 mm) was situate
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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 and 66: electrostatic fields, that could ge
Page 67 and 68: Theory Papers 1. V. Adamenko & V.I.
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: The expression in the exponent of (
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
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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
Page 139 and 140:
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
Page 157 and 158:
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
Page 183 and 184:
Theory of Low-Energy Deuterium Fusi
Page 185 and 186:
If mobile deuterons in a metal are
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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
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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
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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
Page 257 and 258:
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
Page 277 and 278:
The evolution of protoscience into
Page 279 and 280:
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
Page 297 and 298:
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
Page 309 and 310:
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
Page 323 and 324:
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
Page 343 and 344:
Author Index Pages are in Volume 1
Page 345:
Wang, J., 299 Watanabe, A., 338 Wei
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