Volume 2 - LENR-CANR

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Figure 2. Illustration demonstrating spillover effect pumping Figure 2 shows how A&Z quantify the hydrogen absorption behavior of Pd-black by measuring its ability to absorb inflowing H2 at low pressure. In a standard test a constant ccatm/min of H2 gas flows into a vessel of known volume. The pressure-rise time history of powder samples is compared with the pressure rise of the empty test vessel. When the test sample is Ni powder, the pressure rise is faster than for the empty vessel, partially due to inertly occupied volume. When the sample is Pd-filings, there is a small lag in the pressure rise due to the Pd absorption of H2. When the test sample is Pd-black, there is initially no measured rise in pressure, presumably due to immediate transfer of adsorbed H throughout the catalyst bed, accompanied by its rapid absorption within the individual nanometal grains. The duration of the spillover effect period has been used by A&Z to identify good catalyst for fusion promotion. Figure 3. A&Z excess heat run published in 1994 745
The top portion of Fig. 3 shows plots of output power, input power, and cell voltage vs. run time. Fig. 2 bottom shows excess power = output minus input power vs. run time. The period of zero excess power between times A and B is called the incubation period. Figure 4. Electrolysis cell and DS-cathode used in 1995. DS-cathode shown on right. Figure 5. Stainless steel (ss) manifold system used in analysis of desorbed gases 746
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
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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
Page 19 and 20:
Experiments on stimulation of cavit
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foil (thickness 0.1 mm) was situate
Page 23 and 24:
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
Page 85 and 86:
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
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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
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: A&Z introduced new terms to describ
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
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