2002/10/31 by Josiph Mladenov Rangelov, Rangelov, Josiph Mladenov
Physics and Astronomy · #FOS: Physical sciences #Quantum Mechanics and Applications #Quantum Physics (quant-ph) #Quantum and Classical Electrodynamics #Quantum, superfluid, helium dynamics #quant-ph
paper · pdf · doi:10.48550/arxiv.quant-ph/0210208
LaTeX, 17 pages, without pictures
arxiv created 2002/10/31 · openalex publication_date 2002/10/31 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
A physical model of the fluctuating vacuum (FlcVcm) and the photon as an elementary collective excitation in a solitary needle cylindrical form are offered. We assume that the FlcVcm is consistent by neutral dynamides, which are streamlined in a close-packed crystalline lattice. Every dynamide is a neutral pair, consistent by massless opposite point-like elementary electric charges (ElmElcChrgs): electrino (-) and positrino (+). In an equilibrium position two contrary Pnt-Lk ElmElcChrgs within every one dynamide are very closely installed one to another and therefore its aggregate polarization and its ElcFld also have zero values. However the absence of a mass in a rest of an electrino and positrino makes possible they to display an infinitesimal inertness of their own QntElcMgnFlds and a big mobility, what permits them to be found a bigger time in an unequilibrium distorted position. The aggregate ElcFld of dynamide reminds us that it could be considered as the QntElcFld of an electric quasi-dipole because both massless electrino and positrino have the same inertness. The aggregate ElcFld of every dynamide polarizes nearest neighbour dynamides in an account of which they interact between them-self, on account of which their photons display a wave character and behaviour. In order to obtain a clear physical evidence and true physical explanation of an emission and absorption of RlPhtns, I use Fermi method for the determination of the time dependence of expansion coefficients of wave function of SchEl in a hybrid state, using the solution of the Schrodinger quadratic differential wave equation in partial derivatives with the potentials of Coulomb and of Lorentz friction force.