Jones,
                I think the relativistic interpretation of Casimir effect fits 
your hypothesis better but understand your statement "acceleration of any kind 
can increases between Casimir plates or walls because the vacuum energy-density 
is lower inside than outside the cavity." Is a less controversial way to 
introduce your idea. I have posted an abridged blog that focuses only on the 
Casimir effect at
http://froarty.scienceblog.com/16/relativistic-interpretation-of-casimir-effect/
Regards
Fran

From: Jones Beene [mailto:[email protected]]
Sent: Friday, June 11, 2010 12:15 PM
To: [email protected]
Subject: [Vo]:Nickel O-P fusion and beta decay (corrected)

The following is a continuation of a formative hypothesis for the excess energy 
release in one category of LENR involving nickel as the active host; and in 
particular the Arata-Zhang results and numerous replications. The key insight 
is the Oppenheimer-Phillips effect, operating within the confines of a Casimir 
cavity on a specific isotope of nickel.

Arata and Zhang demonstrated, in a remarkable low-powered (unpowered) 
experiment, a stronger excess heat effect in nickel than in palladium; but an 
alloy of nickel with about 15% Pd seems to be optimum. The key to his success 
is probably related to nanostructure - but it highlights the fact that nickel 
is likely to be the better choice for the host matrix in any kind of LENR, 
especially when alloyed, and for the reasons independent of geometry, to be 
outlined below.

The logic of that observation is that an essentially unpowered experiment, 
which has been reproduced by at least six groups to date (two yet to be 
published) must imply that when power is added, the gain will be multiplied. 
This obvious "next step" is underway in a few labs and in particular the Rossi 
energy amplifier, which has been rumored to be successful.

The further hope is that a combination of nanostructure, Casimir cavity 
optimization, outside energy input and direct energy conversion can be 
anticipated to push the results of a hybrid reactor closer to the level of what 
will be required for the long-awaited commercial application ... even if that 
first product only involves mundane space heating. In any event, this is a wide 
open area of research due to the range of prior art, overlap with Mills' 
hydrino theory, which is non-nuclear, and expired patents.

In a prior version of this hypothesis there was an incorrect focus on so-called 
"halo nuclei" which are nuclei having excess neutrons, teetering on the edge of 
nuclear stability. As it turns out, there is no need to invoke this modality. 
The well-known Oppenheimer-Phillips (O-P) effect will suffice to explain most 
of the experimental results, especially when it is considered to operate with 
an appropriate acceleration cavity - or with relativistic (time distortion) 
effects.

Stated simply, acceleration of any kind can increases between Casimir plates or 
walls because the vacuum energy-density is lower inside than outside the 
cavity. A "dissolved" deuteron which is exiting from a nickel matrix into a 
cavity experiences a strong venturi effect, and the rate of acceleration itself 
then increases to the extent necessary to push the deuteron into the inner 
shell of a nickel "target", located on the opposite wall - from whence electron 
shell a "slingshot" effect can electrostatically push the deuteron close to the 
nucleus, overcoming Coulomb repulsion with the help of O-P shielding.

The first relevant fact is that over two-thirds of natural nickel is the 
isotope 58Ni, which has very high nuclear stability - but there is also a ~1% 
isotope: 64Ni which is 6 a.m.u. or ~11% heavier. This is the highest percentage 
of excess neutrons (compared to the most stable isotope) for any transition 
metal in the Periodic Table; but that fact alone does not imply metastability, 
such as in the case of true halo nuclei. From there on, "facts" fade and the 
explanation offered is to a large part contingent on how well it explains 
experimental results.
If we look into the precise mechanics of the Oppenheimer-Phillips effect, it is 
clear that it might not explain actual experimental results with 58Ni or 60Ni 
the majority isotopes - but that it does work with 64Ni as the target. The 
larger issue then resolves to: is there a mechanism that favors the anomalously 
"heavy nickel" isotope, in promoting this effect ? Whether or not there is 
anything special about the extra level of neutrons, such as a presumed 
near-field shielding of positive nuclear charge is unknown. There is some logic 
but no proof that a partially shielded near-field, as would be seen by an 
approaching deuteron in the range of angstroms, is beneficial for the O-P 
effect only with that isotope; or that excess neutrons do provide that close 
shielding which statistically favors the O-P effect for 64Ni, as opposed to the 
other isotopes which are less shielded.

The Oppenheimer-Phillips process, or "stripping reaction", is a type of 
deuteron-induced nuclear reaction which depends on charge shielding of another 
kind. In this process, the neutron component of an approaching deuteron fuses 
with a target nucleus, transmuting the target to a heavier isotope, while 
ejecting the proton. An example, discovered over 85 years ago, is the nuclear 
transmutation of carbon-12  to carbon-13 at lower than expected energy.

The semantic distinction should be made that this is a fusion reaction, 
followed by beta day of the heavier nucleus. The fusion is between deuterium 
and nickel. The ash is a immediate proton, and eventually a beta particle and a 
transmuted element (to copper in the case of 65Ni). Gamma radiation, even if 
secondary, should be apparent. The mechanics of interaction allow a nuclear 
fusion interaction to take place at lower energies than would be expected from 
a calculation of the Coulomb barrier between a deuteron and a target nucleus.

This is because - as a deuteron approaches the positively charged target 
nucleus, it experiences a charge polarization where the "proton-end" faces away 
from the target and the "neutron-end" faces towards the target. The deuteron 
must be accelerated of course, but the rate of acceleration, being a function 
of time, is expected to be influenced by time distortion within a Casimir 
cavity. In this hypothesis, the Casimir cavity of 2-10 nm is a sine qua non for 
success. The fusion proceeds when the binding energy of the approaching neutron 
and the target nucleus exceeds the binding energy of the deuteron and its 
trailing proton. This is a QM reaction which may be statistically altered due 
to time distortion. The split proton is then repelled from the new heavier 
nucleus. This is one indicia of the reaction - hydrogen in place of deuterium 
which will show up in an assay of gases at the end.

Putting this reaction into the context of nickel: with the 58Ni, the O-P effect 
would give 59Ni as the activated nucleus - but this has a very long half-lie - 
thousands of years so that does not help us very much. However, with 64Ni you 
get 65Ni as the activated nucleus and it has a 2.5 hr half life and decays to 
copper. This is the range half-life that can explain "heat after death" and 
also the delay in heat buildup over time, and also a transmutation product 
which has been witnessed in prior LENR results.

This hypotheses should be falsifiable in several ways. Among them is that the 
copper isotope which is the transmutation product is the lesser of copper's two 
isotopes, and that would be an excellent indicator. There should be a small 
direct gamma signature, and beta electrons will leave a predictable spectrum of 
bremsstrahlung radiation that should be detected, and there should be hydrogen 
ash in the deuterium gas after a run which is commensurate with the excess 
energy seen. All of these expected indicia give hope that the O-P/Casimir 
hypothesis will either be confirmed or falsified soon.

Jones

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