Volume 2 - LENR-CANR

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Figure 3. Diode being prepared. We developed another procedure using a nylon plastic tube with brass end fittings. Each metal cap contains a strong spring, which compress the powder. The whole device is protected by another polypropylene tube (Fig. 1). We used Swagelok valves at each end. Figure 4. Second generation devices. 699
Results A. Self-sustained voltage Once the D2 is introduced to our device, voltage quickly rises from zero to 0.5V. To exclude environmental noise, we first use argon as the cell gas and log the cell for a week, following the argon the cell is evacuated, then filled with H2, and left for a second week. The H2 is then removed from the cell, which is evacuated and then filled with D2, and run for a week. The results are shown in Fig. 5. 600 500 400 300 200 100 -100 Cell G1 Ar/H2/D2 0 1 53 105 157 209 261 313 365 417 469 521 573 625 677 729 781 833 885 937 989 1041 1093 1145 1197 1249 1301 1353 1405 1457 1509 1561 1613 1665 1717 1769 1821 1873 1925 1977 2029 2081 2133 2185 2237 Figure 5. Voltage rise with D2 and H2 We conducted a triple-blind test with each diode. The triple-blind results on the chart followed a three week test period. A week on Argon, during which no voltage was observed, a week on H2, which showed a level of voltage, and a week of D2 which showed a higher level of voltage. The argon experiment demonstrated that factors such an external electrical energy, or some galvanic action between the powders of the cell are not the reason for the voltage. However obviously, as a voltage was seen with the H2 some hydrogen oxidation can not be ruled out. We know that the H2 is impure, and there is always 0.03% deuterium present in the gas (mainly in the form of HD molecules). In the palladium, HD dissociate, and we think that the 700 Ar H2 D2 Linear (H2) Linear (D2)
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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
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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
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Theory of Low-Energy Deuterium Fusi
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If mobile deuterons in a metal are
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allowed since [Z1/m1] = [Z2/m2], an
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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
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A simple specific form of beff (p)
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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: We propose that in this field of on
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
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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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