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Figure 1. Polar representation of the 2-D reciprocal space in which the 2-D PSD is defined; the light blue areas indicate the domains on which the PSD2D is averaged to compute the Radial Power Spectral Density (Fig. 1a), the Angular Power Spectral Density (Fig. 1b) and the Maximum Power Spectral Density (Fig. 1c). The analysis has been repeated for different images taken on different sample points (within the same crystal grain), showing similar results within the same crystal grain. Because of the finite sampling rate and limited scale length of the digital AFM images, the computed PSD functions are band-limited over the space of wave-vectors k. In particular, the low frequency cutoff is determined by the scan length, while the high frequency limit is determined by the sampling rate and by the tip geometry. In the present work, the typical wavevector range is 0.2 – 30m -1 . Results and Discussion The Power Spectral Density spectra of samples giving excess heat have been computed to look for common features. A preliminary screening of the data has outlined a particular “multipeaked” structure in the Maximum Power Spectral Density function of the samples that gave excess heat (see Fig. 2 right), while this feature was not observed in the samples that did not give excess heat (see Fig. 3 right). The peak intensities of the analyzed features scale with the peak wave number, which ranges from 1 to 4 m -1 . The similarity in the R@max(|k|) spectrum is indicative of the presence of a pseudo-periodic texture embedded in the surface morphology, with a period in the range of some tenths of microns. Furthermore, as can be seen in Table I, the maximum PSD peak intensity shows a good correlation with the excess heat percentage and reproducibility (when applicable), but it is much lower in the spectra of samples which did not produce excess heat. A similar correlation does not appear to be evident in the specific surface area values, which are shown in Table II and which are scattered less than 10% around the same mean value. 440
RPSD@ max (x10 -32 m 4 ) 0.20 0.10 0.00 L46 2 4 6 8 10 wavevector modulus k (m-1) RPSD@ max (x10 -32 m 4 ) 0.8 0.6 0.4 0.2 L5 2 4 6 8 10 wavevector modulus k (m-1) Figure 2. Top: 3-D AFM images of samples L46, L5 and #64, which gave excess heat during electrochemical deuterium loading; Bottom: Maximum Power Spectral Density curves computed from the AFM images shown on the top RPSD@ max (x10 -32 m 4 ) 0.20 0.15 0.10 0.05 0.00 L47 (point 1) L47 (point 2) L47 (point 3) 2 4 6 8 10 wavevector modulus k (m-1) RPSD@ max (x10 -32 m 4 ) 0.20 0.15 0.10 0.05 0.00 2 4 6 8 10 wavevector modulus k (m-1) Figure 3. Top: 3-D AFM images of samples L47, L51 and L53, which did not give excess heat during electrochemical deuterium loading; Bottom: Maximum Power Spectral Density curves computed from the AFM images shown on the top; in case of sample L47 the curves obtained by the analysis of three different sample points are also shown. 441 L51 RPSD@ max (x10 -32 m 4 ) RPSD@ max (x10 -32 m 4 ) 1.2 #64 1.0 0.8 0.6 0.4 0.2 0.20 0.15 0.10 0.05 0.00 2 4 6 8 10 wavevector modulus k (m-1) L53 2 4 6 8 10 wavevector modulus k (m-1)
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: fundamental peak; on the other hand
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 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
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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
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
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10. A.De Ninno et al. Europhysics L
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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
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of the weak coupling matrix element
Page 163 and 164:
Figure 3. Energy levels that contri
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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
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energetic particles are produced, o
Page 173 and 174:
15. K. Kunimatsu, N. Hasegawa, A. K
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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
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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
Page 187 and 188:
allowed since [Z1/m1] = [Z2/m2], an
Page 189 and 190:
traps (in 3g of Pd particles with a
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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)
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Nuclear Transmutations in Polyethyl
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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
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T+T Fusion CrossSection (Barn) T+T
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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
Page 219 and 220:
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
Page 227 and 228:
Introduction to Challenges and Summ
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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
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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
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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
Page 251 and 252:
Results A. Self-sustained voltage O
Page 253 and 254:
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
Page 283 and 284:
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
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
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[The protocol for producing the ZrO
Page 309 and 310:
Figure 5A. Comparison of generation
Page 311 and 312:
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
Page 329 and 330:
Preparata Prize Acceptance Speech I
Page 331 and 332:
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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