Conservative Relativity Principle and Relevant Physics: Difference between revisions
Imported from text file |
Imported from text file |
||
| Line 8: | Line 8: | ||
==Abstract== | ==Abstract== | ||
Classical electromagnetic field consists of bound and radiation components and only their sum provides for the implementation of energy-momentum conservation of interacting classical charges. Now he focuses on the quantum systems of electrically bound charges which do not radiate in the stationary state and thus their EM field comprises only the bound component. The non-applicability of Maxwell?s equations to quantum mechanics does not permit, in general, ignoring the problem of the energy-momentum conservation for such pure bound E-M field systems and he explores this problem within Schr?dinger-Dirac quantization equation.[[Category:Scientific Paper]] | Classical electromagnetic field consists of bound and radiation components and only their sum provides for the implementation of energy-momentum conservation of interacting classical charges. Now he focuses on the quantum systems of electrically bound charges which do not radiate in the stationary state and thus their EM field comprises only the bound component. The non-applicability of Maxwell?s equations to quantum mechanics does not permit, in general, ignoring the problem of the energy-momentum conservation for such pure bound E-M field systems and he explores this problem within Schr?dinger-Dirac quantization equation. | ||
[[Category:Scientific Paper|conservative relativity principle relevant physics]] | |||
[[Category:Relativity]] | [[Category:Relativity]] | ||
Revision as of 12:11, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | Conservative Relativity Principle and Relevant Physics |
| Author(s) | Alexander L Kholmetskii |
| Keywords | {{{keywords}}} |
| Published | 2010 |
| Journal | None |
Abstract
Classical electromagnetic field consists of bound and radiation components and only their sum provides for the implementation of energy-momentum conservation of interacting classical charges. Now he focuses on the quantum systems of electrically bound charges which do not radiate in the stationary state and thus their EM field comprises only the bound component. The non-applicability of Maxwell?s equations to quantum mechanics does not permit, in general, ignoring the problem of the energy-momentum conservation for such pure bound E-M field systems and he explores this problem within Schr?dinger-Dirac quantization equation.