Volume 2 - LENR-CANR

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the DS-Cathode, D/H is generated within the electrolytic solution of D2O/H2O, i.e., within the Cathode. The generation of D/H corresponds to the presence/absence of the solid fusion reaction. In the former case where D is used, anything other than a small amount of chemical reaction heat cannot be recognized. Figure 4. Heat Generation for H2 Introduction The comparison between D and H is made from the viewpoint of the nuclear fuel, using a newly developed “practical use reactor”(“Solid Reactor”). In the case where D is used, an intensive reaction ( 4 He and thermal energy) due to the solid fusion occurs for both the “verification reactor” and the “Solid Reactor”. On the other hand, in the case where H is used as shown in Figure 4 and Figure 7[A], [B], chemical reaction heat is generated, but 4 He is not generated at all. 757
Figure 5A. Comparison of generation characteristics of Nuclear fusion during “Skirt-Fusion” zone for each fuel (0~300min) Figure 5B. Comparison of generation characteristics of Nuclear fusion during “Skirt-Fusion” zone for each fuel (after 300min) 758
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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
Page 31 and 32:
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
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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
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
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: [The protocol for producing the ZrO
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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