Conservative Relativity Principle and Relevant Physics: Difference between revisions
Imported from text file |
Fill in keywords from the wiki's abstract records |
||
| (2 intermediate revisions by 2 users not shown) | |||
| Line 2: | Line 2: | ||
| title = Conservative Relativity Principle and Relevant Physics | | title = Conservative Relativity Principle and Relevant Physics | ||
| author = [[Alexander L Kholmetskii]] | | author = [[Alexander L Kholmetskii]] | ||
| keywords = relativity principle, electromagnetic field, quantum mechanics, conservation, momentum | |||
| published = 2010 | | published = 2010 | ||
}} | }} | ||
| Line 12: | Line 12: | ||
[[Category:Scientific Paper|conservative relativity principle relevant physics]] | [[Category:Scientific Paper|conservative relativity principle relevant physics]] | ||
[[Category:Relativity]] | [[Category:Relativity|conservative relativity principle relevant physics]] | ||
Latest revision as of 07:28, 21 July 2026
| Scientific Paper | |
|---|---|
| Title | Conservative Relativity Principle and Relevant Physics |
| Author(s) | Alexander L Kholmetskii |
| Keywords | relativity principle, electromagnetic field, quantum mechanics, conservation, momentum |
| Published | 2010 |
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.