Sometimes I have similar feelings Eric.  The evidence seems to suggest that He4 
can form and release its massive energy in a milder manner than is typical.  I 
suppose that we should be trying to understand why the normal fusion paths lead 
to the emission of a proton or neutron generally with the gamma as the rare 
case.


The behavior seen under hot fusion conditions is perhaps the strange one since 
He4 has such strong binding energy when compared against the two other main 
combinations.  You appear to harbor the feeling that coupling to nearby fields 
might be the key reason for the vast difference and I likewise wonder.  Hot 
fusion conditions are such that there are no nearby nuclei available to 
originate the coupling fields and there are certainly no heavy metallic ones to 
help.


Some of the recent reports tend to suggest that very strong magnetic fields 
might get into the act, especially according to the recent demonstration by 
DGT.  The strengths of these large external fields begs the question  as to 
just how strong the components of the fields are at the atomic size range.  
Maybe they come into play at the extremes and allow the relatively large energy 
to be released into a much larger region than expected.  What would be a better 
suppression technique than to eliminate the generation of the normally 
energetic gammas in the first place.


Dave



-----Original Message-----
From: Eric Walker <[email protected]>
To: vortex-l <[email protected]>
Sent: Mon, Dec 2, 2013 11:17 pm
Subject: Re: [Vo]:Re:



On Sun, Dec 1, 2013 at 11:56 PM, P.J van Noorden <[email protected]> wrote:



Now comes the big question. Are there any new nuclear reactions possible which 
produce for instance 4He without particles or gamma emission? 




I'm thinking we've made the missing gamma problem harder than it needs to be.  
My guess -- there's genuine d+d and p+d fusion going on (as well as the 
occasional transmutation), and when a fusion happens, instead of the usual, 
slow gamma emission, there's a near-instantaneous transfer of electrostatic 
energy to the nearby electron cloud in the host metal.  If this is what 
happens, the energy of the short-lived unstable daughter can be expected to be 
divided between a large number of surrounding electrons, giving rise to a bath 
of lower-energy photons rather than a single high-energy gamma photon, together 
with a near motionless stable daughter.


Eric




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