This idea of fractioning the energy is similar to the scheme that Takahashi described in his TSC theory. Be-8* splits into two He* which decay to ground state with a little kinetic energy and a lot of low energy photons taken up by the lattice. Takahashi make the point that the coupling of the He* during decay to the lattice needs more work. This was in 2010. I do not know whether he has finished the coupling mechanism.
I too was surprised at Haglestein's obvious neglect of the spin issues in the presentation of his theory at his 5th day session just recently. I have a similar idea for the Ni-H system--a proton-electron pair is positioned near a Ni on the surface or in a crack and the combined virtual particle (Ni Nucleus and proton-electron pair) reacts to form a new nucleus. The following may be what happens: The new Ni "daughter" decays as it will to copper or whatever. Ni-59 gives off it positron and the positron-electron initiation occurs with its .51 mev gammas. However with the proper temperature and black body background radiation for the Ni system the system favors reactions that distribute energy to the lattice or other Ni nuclei via spin coupling, and the Ni-59 may not form with the reaction ending up with Cu-59 directly, avoiding the positron associated radiation. The black body background radiation, having an entire spectrum of oscillating electro-magnetic fields in all directions, interact with Ni nuclei via their magnetic moments at the resonant frequencies making the release of many quanta possible from each excited Ni nucleus during the fractionation required by the main transition with its loss of mass. Here again the virtual Ni* first exists in a high spin energy state and decays via spin coupling to the other activated nuclei in the local system. A local temperature increase changes the reaction probability so that no more than one reaction occurs at a time and the system does not destroy itself. Other surfaces and cracks act the same way with a frequency controlled by the temperature. A time constant is associated with the change in the black body radiation spectrum and does not allow coupling of too many Nuclei at the same time given the constant removal of the resonant photons needed to activate the spin states of the Ni nuclei. Axil probably can add some obvious steps that I have omitted.(:-) Bob ----- Original Message ----- From: Eric Walker To: [email protected] Sent: Wednesday, March 05, 2014 10:10 PM Subject: Re: [Vo]:"Christopher H. Cooper" On Wed, Mar 5, 2014 at 5:09 PM, Edmund Storms <[email protected]> wrote: When alpha particles pass through material, a series of nuclear reactions can occur that emit radiation. In addition, bremsstrahlung radiation is emitted as the alpha slows down. Hagelstrin describes these processes in the papers I attached previously. I suggest you read them. If an alpha is born from a [dd]* resonance in which the mass energy is fractionated among a large number of sinks (e.g., nearby electrons and ion cores), the 4He daughter would have no or almost no energy. There would be the bath of photons from the fractionation, the nearly stationary 4He daughter, and no Bremsstrahlung from collisions by a fast particle. Eric
