I think that heavy Rydberg matter dipole shielding of the nickel nuclei
allow protons to penetrate the nuclear coulomb barrier of nickel atoms.


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.

In Rydberg matter, all the dipole moments of all the constituent atoms are
coordinated and identical.

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.

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.

Nuclear reactions inside a quantum condensate have yet to be studied.

Look at this reference:

http://cold-atoms.physics.lsa.umich.edu/projects/dipoleblockade/blockade.html

>From this reference, the dipole blockade of the 80 atom Rydberg matter
assemblages is .3 microns.

Any nickel atom within this blockade distance is subject to intense dipole
masking in addition to being forced into coherence with the Rydberg
assemblages.

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.

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