Conservative Relativity Principle and Relevant Physics - Revision history

ClaudeBot: restore accented characters lost to the encoding bug (verified names/words only; URLs untouched)

2026-07-22T13:19:59Z

restore accented characters lost to the encoding bug (verified names/words only; URLs untouched)

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	==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.		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 Schrödinger-Dirac quantization equation.

	[[Category:Scientific Paper\|conservative relativity principle relevant physics]]		[[Category:Scientific Paper\|conservative relativity principle relevant physics]]

	[[Category:Relativity\|conservative relativity principle relevant physics]]		[[Category:Relativity\|conservative relativity principle relevant physics]]

ClaudeBot: fix apostrophes lost to the character-encoding bug (Einstein?s -> Einstein's); URLs left untouched

2026-07-22T13:03:43Z

fix apostrophes lost to the character-encoding bug (Einstein?s -> Einstein's); URLs left untouched

← Older revision		Revision as of 09:03, 22 July 2026
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	==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.		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:Scientific Paper\|conservative relativity principle relevant physics]]

	[[Category:Relativity\|conservative relativity principle relevant physics]]		[[Category:Relativity\|conservative relativity principle relevant physics]]

ClaudeBot: Fill in keywords from the wiki's abstract records

2026-07-21T11:28:25Z

Fill in keywords from the wiki's abstract records

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	\| 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
	}}		}}

ClaudeBot: Remove empty None journal/publisher placeholder (dead red-link cleanup)

2026-07-18T23:33:26Z

Remove empty None journal/publisher placeholder (dead red-link cleanup)

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	\| author = [[Alexander L Kholmetskii]]		\| author = [[Alexander L Kholmetskii]]
	\| published = 2010		\| published = 2010
	~~\| journal = [[None]]~~
	}}		}}

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2017-01-02T02:24:46Z

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	[[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]]

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2017-01-01T17:11:10Z

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	==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]]

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2016-12-30T16:24:45Z

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{{Infobox paper
| title = Conservative Relativity Principle and Relevant Physics
| author = [[Alexander L Kholmetskii]]
| 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.[[Category:Scientific Paper]]

[[Category:Relativity]]