Uravnyeniya dvizhyeniya Gai{cyrillic, short}zyenbyerga v protsyedurye Kaldiroly-Montal{cyrillic small soft sign}di

Jannussis, A; Leodaris, A; Filippakis, P; Filippakis, Th; Zisis, V

dc.contributor.author	Jannussis, A	en
dc.contributor.author	Leodaris, A	en
dc.contributor.author	Filippakis, P	en
dc.contributor.author	Filippakis, Th	en
dc.contributor.author	Zisis, V	en
dc.date.accessioned	2014-03-01T01:38:25Z
dc.date.available	2014-03-01T01:38:25Z
dc.date.issued	1982	en
dc.identifier.issn	03693554	en
dc.identifier.uri	https://dspace.lib.ntua.gr/xmlui/handle/123456789/22136
dc.title	Uravnyeniya dvizhyeniya Gai{cyrillic, short}zyenbyerga v protsyedurye Kaldiroly-Montal{cyrillic small soft sign}di	en
heal.type	journalArticle	en
heal.identifier.primary	10.1007/BF02721159	en
heal.identifier.secondary	http://dx.doi.org/10.1007/BF02721159	en
heal.publicationDate	1982	en
heal.abstract	In this paper the procedure of Caldirola and Montaldi is applied in the Heisenberg representation. It is also proved here that the introduction of the parameter τ contributes to the specification of a quantum-dissipative system, as exactly happens in the Schrödinger representation. As an example the case of the harmonic oscillator as well as that of the damped harmonic oscillator are examined. © 1982 Società Italiana di Fisica.	en
heal.publisher	Società Italiana di Fisica	en
heal.journalName	Il Nuovo Cimento B	en
dc.identifier.doi	10.1007/BF02721159	en
dc.identifier.volume	67	en
dc.identifier.issue	2	en
dc.identifier.spage	161	en
dc.identifier.epage	172	en