Classical Model of Rutherford-Santilli Neutron

Model n(RS), isomer of n, Bohr's real ground state of H$^{+}$: proton p and electron e, separated 0.81 Fermi, in circular orbits about c.m., with parallel magnetic dipole moments (MDMs) normal to orbital plane. Binding force: Coulomb less magnetic. Each momentum: mass x velocity less charge x (vector potential A at particle). Assuming unmutated p, and n data: orbital e velocity v is 0; slight mutation: v/c $<<<$ 1. (Ref. 1.) Mutated e: mass, 2.5 x (mass of free e); spin, 0.038$\hbar$/2; g, 0.52; MDM, 3.6 x E(-26) S.I. Stability requires external A, 0[0.01 S.I.], found in atomic nuclei. The n(RS) \textbf{$\to $} n by spin flip of e; e captured by positive constituent of p; gamma photon emitted. (Ref. 2.) \newline \newline 1. R. M. Santilli, \textit{Hadronic Journal 13}, 513 (1990); \textit{Chinese Journal Sys. Eng. {\&} Elec. 6}, No. 4, 177 (1995) \newline 2. R. B. Driscoll, \textit{Hadronic Journal 27}, No. 6 (2004)