dorsal/arxiv
View SchemaPhysical Model of the Fluctuating Vacuum and Photon as its Elementary Excitation
| Authors | Josiph Mladenov Rangelov |
|---|---|
| Categories | |
| ArXiv ID | quant-ph/0210208 |
| URL | https://arxiv.org/abs/quant-ph/0210208 |
Abstract
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.
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"abstract": "A physical model of the fluctuating vacuum (FlcVcm) and the photon as an\nelementary collective excitation in a solitary needle cylindrical form are\noffered. We assume that the FlcVcm is consistent by neutral dynamides, which\nare streamlined in a close-packed crystalline lattice. Every dynamide is a\nneutral pair, consistent by massless opposite point-like elementary electric\ncharges (ElmElcChrgs): electrino (-) and positrino (+). In an equilibrium\nposition two contrary Pnt-Lk ElmElcChrgs within every one dynamide are very\nclosely installed one to another and therefore its aggregate polarization and\nits ElcFld also have zero values. However the absence of a mass in a rest of an\nelectrino and positrino makes possible they to display an infinitesimal\ninertness of their own QntElcMgnFlds and a big mobility, what permits them to\nbe found a bigger time in an unequilibrium distorted position. The aggregate\nElcFld of dynamide reminds us that it could be considered as the QntElcFld of\nan electric quasi-dipole because both massless electrino and positrino have the\nsame inertness. The aggregate ElcFld of every dynamide polarizes nearest\nneighbour dynamides in an account of which they interact between them-self, on\naccount of which their photons display a wave character and behaviour. In order\nto obtain a clear physical evidence and true physical explanation of an\nemission and absorption of RlPhtns, I use Fermi method for the determination of\nthe time dependence of expansion coefficients of wave function of SchEl in a\nhybrid state, using the solution of the Schrodinger quadratic differential wave\nequation in partial derivatives with the potentials of Coulomb and of Lorentz\nfriction force.",
"arxiv_id": "quant-ph/0210208",
"authors": [
"Josiph Mladenov Rangelov"
],
"categories": [
"quant-ph"
],
"title": "Physical Model of the Fluctuating Vacuum and Photon as its Elementary Excitation",
"url": "https://arxiv.org/abs/quant-ph/0210208"
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