Kitamura, A., 195, 400 Knies, D., (Vol. 2) 444 Knies, D. L., (Vol. 2) 429, (Vol. 2) 437 Kornilova, A., (Vol. 2) 418 Kowalski, L., (Vol. 2) 723 Kozima, H., (Vol. 2) 613, (Vol. 2) 618 Krakov, V., 106 Lautzenhiser, T. V., 53 Lecci, S., (Vol. 2) 429, (Vol. 2) 437, (Vol. 2) 444 Lesin, S., 106 Letts, D., 71, 333 Li, J., 299 Li, X., (Vol. 2) 623, (Vol. 2) 780 Lipson, A., 220, (Vol. 2) 780 Little, M., 47 Little, S., 47 Liu, B., (Vol. 2) 623 Lu, X., 328 Luce, G., 47 Lyakhov, B., 220 Mancini, A., 385 Marchesini, M., 385 Marini, P., 385 Marmigi, A., 385 Martini, U., 385 Mastromatteo, U., 385 McConnell, M., 288 McKubre, M., 32, (Vol. 2) 444, (Vol. 2) 673 Melich, M., 220, (Vol. 2) 586, (Vol. 2) 596, (Vol. 2) 704 Meulenberg, A., 633 Miles, M., 6, (Vol. 2) 766 Miley, G. H., 212, (Vol. 2) 451 Mizuno, T., 147 Motohiro, T., 203 Murase, A., 203 Murat, D., 60, (Vol. 2) 546 Nakamura, M., 385 Nohmi, T., 195, 400 Oriani, R. A., 250 Ozaki, M., 338 Passell, T., (Vol. 2) 737 793 Phelps, D. W., 53 Purchi, E., 385 Righi, E., 385 Roussetski, A., 220 Rufoloni, A., (Vol. 2) 444 Sansovini, M., (Vol. 2) 429, (Vol. 2) 437, (Vol. 2) 444 Sarto, F., (Vol. 2) 429, (Vol. 2) 437, (Vol. 2) 444 Sasabe, S., 338 Sasaki, Y., 195, (Vol. 2) 400 Saunin, E., 220 Sawada, S., 147 Scanlan, B., 263 Scaramuzzi, F., (Vol. 2) 780 Seto, R., 400 Shapiro, A., 106 Shen, B. J., 328 Sinha, K., (Vol. 2) 633 Sona, P. G., 385 Spallone. A., 385 Srinivasan, M., (Vol. 2) 780 Storms, E., 11, 263 Stringham, R., (Vol. 2) 411 Swartz, M., 123, 343, (Vol. 2) 458, (Vol. 2) 497, (Vol. 2) 639, (Vol. 2) 653, (Vol. 2) 689 Sysoev, N., (Vol. 2) 418 Szpak, S., (Vol. 2) 766, (Vol. 2) 772 Takahashi, A., 195, 400, (Vol. 2) 663 Takahashi, N., 203 Taniike, A., 195, 400 Tanzella, F., 32, (Vol. 2) 444 Tian, J., 328 Todarello, F., 385 Toriyabe, Y., 310 Trenta, G., 385 Tsirlin, M., 106 Tsuchiya, K., 338 Verner, G., 343, (Vol. 2) 458 Violante, V., 429, (Vol. 2) 437, (Vol. 2) 444 Vysotskii, V., (Vol. 2) 418, (Vol. 2) 484 Wang, C., 299
Wang, J., 299 Watanabe, A., 338 Wei, Q., (Vol. 2) 623 Weinberg, A., 343 Weng, Z. K., 328 Wu, S., 299 Yamaguchi, T., 195, 400 Yang, X., (Vol. 2) 451 Yao, S., 299 Zhang, H., 299 Zhang, W-S., 26 Zhang, Y-C., (Vol. 2) 752 Zhang, Z-L., 26 Zhao, Y., 299 Zheng, S., (Vol. 2) 623 Zilov, T., 106 794
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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
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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
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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
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The evolution of protoscience into
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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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- 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
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- 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
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- Page 343: Author Index Pages are in Volume 1