Difference between revisions of "Conservative Relativity Principle and Relevant Physics"
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| − | 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. | + | 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:Relativity]] | + | [[Category:Scientific Paper|conservative relativity principle relevant physics]] |
| + | |||
| + | [[Category:Relativity|conservative relativity principle relevant physics]] | ||
Latest revision as of 19:24, 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.
