Physical model of Dirac electron. Calculation of its mass at rest and own electric and magnetic intensities on its moment location

Abstract

The physical model (PhsMdl) of the relativistic quantized Dirac's electron (DrEl) is proposed. The DrEl is regarded as a point-like (PntLk) elementary electric charge (ElmElcChrg), taking simultaneously part in following four disconnected different motions: a/ in Einstein's random trembling harmonic shudders as a result of momentum recoils (impulse kicks), forcing the DrEl's PntLk ElmElcChrg at its continuous emission and absorption of high energy stochastic virtual photons (StchVrtPhtns) by its PntLk ElmElcChrg ; b/ in Schrodinger's fermion vortical harmonic oscillations of DrEl's fine spread (FnSpr) ElmElcChrg, who minimizes the self-energy at a rest of is an electromagnetic self-action between its continuously moving FnSpr ElmElcChrg and proper magnetic dipole moment (MgnDplMmn) and the corresponding potential and vector-potential; All the relativistic dynamical properties of the DrEl are results of the participate of its FnSpr ElmElcChrg in the Schrodinger's fermion vortical harmonic oscillations. c/ in Furthian quantized stochastic boson circular harmonic oscillations as a result of the permanent electric or magnetic interaction of its well spread (WllSpr) ElmElcChrg or proper MgnDplMmn with the electric intensity (ElcInt) or the magnetic intensity (MgnInt) of the resultant quantized electromagnetic field (QntElcMgnFld) of all the StchVrtPhtns within the fluctuating vacuum (FlcVcm); All the quantized dualistic dynamical properties of the SchEl are results of the participate of its WllSpr ElmElcChrg in the Furth's stochastic boson circular harmonic oscillations. d/ in Nweton's classical motion along a clear-cut smooth thin line as a result of some interaction of its over spread (OvrSpr) ElmElcChrg, MgnDplMmn or bare mass with the intensities of some classical fields.