Volume 2 - LENR-CANR

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21. P.A. Mosier-Boss, S. Szpak, F.E. Gordon, and L.P.G. Forsley, ““Use of CR-39 in Pd/D Codeposition Experiments: A Response to Kowalski,” Eur. Phys. J. Appl. Phys., 41 (2008) in press. Earlier we reported that the pits generated in CR-39 detectors during Pd/D co-deposition experiments are consistent with those observed for pits that are of a nuclear origin. Recently, that interpretation has been challenged. In this communication, additional experimental data and further analysis of our earlier results are provided that support our original conclusions. 777
Preparata Prize Acceptance Speech I. Dardik Energetics Technologies P.O.Box 3026 Omer Industrial Park Omer, Israel During ICCF-14, Irving Dardik was awarded the Preparata Medal for 2008. The honor, named after the late Italian physicist Giuliano Preparata, is awarded at ICCF conferences for contributions to progress in Condensed Matter Nuclear Science. Thank you Bill and Mike. I am honored to be this year’s recipient of the Preparata Prize and thank the Committee for this recognition. Back in 1991 I applied for a low energy nuclear reaction patent based on SuperWaves. The United States patent office shelved it along with all the other applications that our community has submitted over the years. In 2001, one brave man, Professor Herman Branover, stepped forward and listened to my predictions that SuperWaves would make a difference in <strong>LENR</strong> results. Next in, was Ehud Greenspan who stated that even if there was a 1% chance that I was right, he would listen. After hearing me out, he upped that percentage to 50% and joined Dr. Branover, Alison Godfrey and me in a meeting with the visionary Sidney Kimmel. In a bold and daring move, Sidney Kimmel committed his personal resources towards funding a SuperWaves laboratory in Israel whose mission was to use SuperWaves to produce usable energy. I am grateful to Alison Godfrey for her extraordinary leadership in building Energetics Technologies into what it is today…. to Shaul Lesin for taking the lead in establishing Energetics in Israel and hiring a team of brilliant scientists in 2001 — 10 long years after my first patent application in this field. Their work is impeccable and has justified Dr. Greenspan’s participation. They have surpassed all expectations of what could be accomplished in a few short years using SuperWaves. By 2003, we presented some of our early results at ICCF 10 and had the honor of drawing the attention of Mike McKubre. Mike’s scientific sophistication and leadership in the DARPA replication projects with SRI, has been invaluable. I also want to thank Vittorio Violante of ENEA and the extraordinary team at NRL. I would like to acknowledge Dave Nagel and Mike Melich for organizing an extraordinary conference, bringing in new faces and presenting the field in a cohesive and well developed way. As Llewellyn King pointed out in his Keynote Address, we are coming off of a summer of skyrocketing energy costs. It is only August, and many in this country and around the world are already in fear; wondering how they will afford to heat their homes this coming winter. 778
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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
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
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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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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: 17. S. Szpak, P.A. Mosier-Boss, and
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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