Terahertz stimulated emission from silicon doped by hydrogenlike acceptors

dc.bibliographicCitation.firstPage21009eng
dc.bibliographicCitation.issue2eng
dc.bibliographicCitation.journalTitlePhysical Review Xeng
dc.bibliographicCitation.lastPage2569eng
dc.bibliographicCitation.volume4eng
dc.contributor.authorPavlov, S.G.
dc.contributor.authorDeßmann, N.
dc.contributor.authorShastin, V.N.
dc.contributor.authorZhukavin, R.K.
dc.contributor.authorRedlich, B.
dc.contributor.authorvan der Meer, A.F.G.
dc.contributor.authorMittendorff, M.
dc.contributor.authorWinnerl, S.
dc.contributor.authorAbrosimov, N.V.
dc.contributor.authorRiemann, H.
dc.contributor.authorHübers, H.-W.
dc.date.accessioned2020-11-12T07:22:18Z
dc.date.available2020-11-12T07:22:18Z
dc.date.issued2014
dc.description.abstractStimulated emission in the terahertz frequency range has been realized from boron acceptor centers in silicon. Population inversion is achieved at resonant optical excitation on the 1Λ8+ → 1Λ7- , 1Λ6-, 1Λ8- intracenter transitions with a midinfrared free-electron laser. Lasing occurs on two intracenter transitions around 1.75 THz. The upper laser levels are the 1Λ7- , 1Λ6- , and 1Λ8- states, and the lower laser level for both emission lines is the 2Λ8+ state. In contrast to n-type intracenter silicon lasers, boron-doped silicon lasers do not involve the excited states with the longest lifetimes. Instead, the absorption cross section for the pump radiation is the dominating factor. The four-level lasing scheme implies that the deepest even-parity boron state is the 2Λ8+ state and not the 1Λ7+ split-off ground state, as indicated by other experiments. This is confirmed by infrared absorption spectroscopy of Si:B.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://doi.org/10.34657/4555
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/5926
dc.language.isoengeng
dc.publisherCollege Park : American Institute of Physics Inc.eng
dc.relation.doihttps://doi.org/10.1103/PhysRevX.4.021009
dc.relation.issn2160-3308
dc.rights.licenseCC BY 3.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/3.0/eng
dc.subject.ddc530eng
dc.subject.otherOpticseng
dc.subject.otherSemiconductor physicseng
dc.subject.otherFree electron laserseng
dc.subject.otherLight absorptioneng
dc.subject.otherNuclear physicseng
dc.subject.otherOpticseng
dc.subject.otherQuantum well laserseng
dc.subject.otherStimulated emissioneng
dc.subject.otherAbsorption cross sectionseng
dc.subject.otherAcceptor centerseng
dc.subject.otherBoron-doped siliconeng
dc.subject.otherDominating factorseng
dc.subject.otherPopulation inversionseng
dc.subject.otherPump radiationeng
dc.subject.otherSemiconductor physicseng
dc.subject.otherTerahertz frequency rangeeng
dc.subject.otherSiliconeng
dc.titleTerahertz stimulated emission from silicon doped by hydrogenlike acceptorseng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorIKZeng
wgl.subjectPhysikeng
wgl.typeZeitschriftenartikeleng
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