Can't have this kookiness.
R(-1) ultradense deuterium is a wonderful & completely unproven, probably unphysical idea. If it exists then CF is easy.
You are talking about real Rydberg matter, which does exist, but is not magical, and therefore does not do what you say. Details below.
Axil wrote:D Tibbets wrote:Axil wrote:
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It has been reported that gamma ray bursts occur at startup and shutdown of high COP Rossi reactor designs. The Rossi process is radiation safe at high temperatures, but will produce gamma rays at low hydrogen envelope temperatures.
To avoid this issue, Rossi has downsized his reactor module to avoid this low temperature window of gamma production venerability.
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I hope it is apparent that a stage where gammas are produced and a stage where gammas are not produced implies, not one, but two different nuclear reaction processes, neither of which are explained.
Dan Tibbets
Tom, please permit me to explain:
I think that heavy Rydberg matter dipole shielding of the nickel nuclei allow protons to penetrate the nuclear coulomb barrier of nickel atoms.
This is pure moonshine. The Rydberg dipoles are large because the electron moves a long distance. Such a large dipole cannot possibly shield a nucleus up ultra-close. It is the opposite of what is needed.
In Rydberg matter, this dipole shielding goes as the 7th power of the number of atoms in the Rydberg matter assemblages. This polarization of Rydberg matter is clearly huge and can easily overcome the coulomb potential in the nickel atoms.
Always worry when somone says "clearly". Huge polarization has no relationship to shielding coulomb potential, see above. If you want to argue, lets do the field equations?
In Rydberg matter, all the dipole moments of all the constituent atoms are coordinated and identical.
What does "coordinated" mean. I think you mean the electron wave functions are coherent. That I agree, at v low temp needed for Rydberg matter.
Furthermore, the coherent nature of Rydberg matter range from just a single atom to large numbers in excess of 100 based upon the temperature and pressure of the hydrogen envelope; the higher the pressure and temperature, the greater on the average is the number of member atoms in the Rydberg matter assemblages. In other words, the higher the temperature of this hydrogen envelope, the greater is the number of coherent atoms that join the Rydberg matter assemblages.
Well no, high temp will break Rydberg matter bonds which are fragile because have low bond energy.
Tom:
You may have not considered how nuclear reactions affect atoms in a large assemblage of coherent and entangled atoms.
In such a collection, what happens to one member of such a coherent collection happens to them all. It may well be that an averaging effect takes place where the nuclear energy output of one atom is averaged over a hundred or more atoms in the coherent collection.
These have (at v low temp) coheent electrons. They are not coherent nuclei. I have not yet seen any suggestion that electron coherence should affect nuclear reactions. There seems no connection.
Nuclear reactions inside a quantum condensate have yet to be studied.
That is like saying nuclear reactions inside HTS wire have yet to be studiedb. So what?
yes
Any nickel atom within this blockade distance is subject to intense dipole masking in addition to being forced into coherence with the Rydberg assemblages.
No to dipole masking. "forced to coherence"? Why would the electrons be forced to coherence? And if they were, as above, so what?
Rydberg matter sits on top of the nano-powder and completely negates coulomb repulsion of the nuclei of these nickel atoms that they cover.
However, when Rydberg coherence is not yet fully established or is breaking down, gamma radiation production will occur, not being completely negated by atomic coherence. This happens when the temperature and/or the pressure of the hydrogen envelope is lowering or low.
This is where the gamma radiation bursts from the Rossi reactor sometimes come from.
This post does not make sense.