DC Field | Value | Language |
---|---|---|
dc.contributor.author | k. an | ko |
dc.contributor.author | m. s. feld | ko |
dc.date.accessioned | 2013-02-28T04:25:05Z | - |
dc.date.available | 2013-02-28T04:25:05Z | - |
dc.date.created | 2012-02-06 | - |
dc.date.created | 2012-02-06 | - |
dc.date.issued | 1997-08 | - |
dc.identifier.citation | PHYSICAL REVIEW A, v.56, no.2, pp.1662 - 1665 | - |
dc.identifier.issn | 1050-2947 | - |
dc.identifier.uri | http://hdl.handle.net/10203/72768 | - |
dc.description.abstract | The recent single-atom microlaser experiment [K. An et al., Phys. Rev. Lett. 73, 3375 (1994)], in which a stream of inverted two-level atoms is injected into an ultrahigh Q cavity, can be understood in the context of a semiclassical four-level laser model. Transit time broadening due to short atom-cavity interaction time effectively introduces nonradiative decay of the two levels in the model. The steady-state solution of semiclassical photon and atom rate equations for the intracavity mean photon number versus the intracavity atom number provides a good fit to the experimental data. | - |
dc.language | English | - |
dc.publisher | Amer Physical Soc | - |
dc.subject | MICROLASER | - |
dc.subject | MASER | - |
dc.title | Semi-classical four-level single atom laser | - |
dc.type | Article | - |
dc.identifier.wosid | A1997XQ61800085 | - |
dc.type.rims | ART | - |
dc.citation.volume | 56 | - |
dc.citation.issue | 2 | - |
dc.citation.beginningpage | 1662 | - |
dc.citation.endingpage | 1665 | - |
dc.citation.publicationname | PHYSICAL REVIEW A | - |
dc.identifier.doi | 10.1103/PhysRevA.56.1662 | - |
dc.contributor.localauthor | k. an | - |
dc.contributor.nonIdAuthor | m. s. feld | - |
dc.type.journalArticle | Article | - |
dc.subject.keywordPlus | MICROLASER | - |
dc.subject.keywordPlus | MASER | - |
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