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dc.contributor.authorTanatar, Bilalen_US
dc.date.accessioned2016-02-08T10:53:36Z
dc.date.available2016-02-08T10:53:36Z
dc.date.issued1994en_US
dc.identifier.issn0038-1098
dc.identifier.urihttp://hdl.handle.net/11693/26005
dc.description.abstractUnder favorable conditions, a new collective mode besides the usual plasmons may exist in degenerate electron-hole liquids. We calculate the dispersion and damping of this new mode (called the acoustic plasmon mode) in a quasi-one-dimensional, two-component electron liquid. We carry out our calculations first within the random-phase approximation, then include the effects of local-field corrections using a Hubbard-like approximation. The latter decreases the acoustic plasmon dispersion. © 1994.en_US
dc.language.isoEnglishen_US
dc.source.titleSolid State Communicationsen_US
dc.relation.isversionofhttp://dx.doi.org/10.1016/0038-1098(94)90456-1en_US
dc.subjectAcoustic dispersionen_US
dc.subjectApproximation theoryen_US
dc.subjectCharge carriersen_US
dc.subjectDampingen_US
dc.subjectLattice vibrationsen_US
dc.subjectMathematical modelsen_US
dc.subjectRandom processesen_US
dc.subjectAcoustic plasmon modeen_US
dc.subjectElectron hole liquidsen_US
dc.subjectHarmonic confinement potentialen_US
dc.subjectElectronsen_US
dc.titleCollective modes in a quasi-one-dimensional, two-component electron liquiden_US
dc.typeArticleen_US
dc.departmentDepartment of Physicsen_US
dc.citation.spage699en_US
dc.citation.epage702en_US
dc.citation.volumeNumber92en_US
dc.citation.issueNumber8en_US
dc.identifier.doi10.1016/0038-1098(94)90456-1en_US
dc.publisherPergamon Pressen_US
dc.contributor.bilkentauthorTanatar, Bilalen_US


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