Bohrs Atom Completed: the Rutherford-Santilli Neutron

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The Rutherford-Santilli neutron n is considered classically, with intrinsic momentums p = mv*-qA* (m:mass; v*:velocity; q:charge; A*:vector potential of or at each particle, electron or proton; *: denotes vector). It is the true ground state of Bohrs hydrogen atom. It is subject to orbital capture. Spin-flip of the electron, then its fusion with a positively charged constituent of the proton and emission of a gamma photon forms a negatively charged constituent of the resultant isomer of n: the conventional neutron n. The assumed existence of n requires that the electron, acted on by the intense magnetic induction field of the proton, be mutated to spin and magnetic dipole moment respectively 0.0379 Plancks constant/4(pi) and 3.58 x 10-26 SIU, with g-factor 0.516. The intrinsic structure of the electron is treated from this standpoint. Stability of n' requires external vector potential fields whose magnitudes are present in the interiors of nuclei. Absent such field strengths, or with spin-flip of the electron (whether quantum mechanical or causally induced by an impacting particle), n becomes n plus a gamma photon.

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