DC Field | Value | Language |
---|---|---|
dc.contributor.author | Jin, YG | ko |
dc.contributor.author | Chang, Kee-Joo | ko |
dc.date.accessioned | 2013-03-02T13:51:24Z | - |
dc.date.available | 2013-03-02T13:51:24Z | - |
dc.date.created | 2012-02-06 | - |
dc.date.created | 2012-02-06 | - |
dc.date.issued | 1999-06 | - |
dc.identifier.citation | PHYSICAL REVIEW B, v.59, no.23, pp.14841 - 14844 | - |
dc.identifier.issn | 0163-1829 | - |
dc.identifier.uri | http://hdl.handle.net/10203/73831 | - |
dc.description.abstract | We investigate the energy-loss spectrum of bce Li through first-principles pseudopotential calculations. Using an N-point Pade approximant, we calculate the dielectric response function and produce the fine structure of the dynamic structure factor, in good agreement with available experimental data. The local-field and exchange-correlation effects are found to be significant in the particle-hole excitation region. The local-field effect gives rise to peaks in the energy-loss spectrum, which are associated with a plasmon-Fano resonance and zone-boundary collective states. | - |
dc.language | English | - |
dc.publisher | AMERICAN PHYSICAL SOC | - |
dc.subject | SIMPLE METALS | - |
dc.subject | COLLECTIVE STATES | - |
dc.subject | RESONANCE | - |
dc.subject | LITHIUM | - |
dc.title | Dynamic response function and energy-loss spectrum for Li using an N-point Pade approximant | - |
dc.type | Article | - |
dc.identifier.wosid | 000081134500006 | - |
dc.identifier.scopusid | 2-s2.0-4243225232 | - |
dc.type.rims | ART | - |
dc.citation.volume | 59 | - |
dc.citation.issue | 23 | - |
dc.citation.beginningpage | 14841 | - |
dc.citation.endingpage | 14844 | - |
dc.citation.publicationname | PHYSICAL REVIEW B | - |
dc.contributor.localauthor | Chang, Kee-Joo | - |
dc.contributor.nonIdAuthor | Jin, YG | - |
dc.type.journalArticle | Article | - |
dc.subject.keywordPlus | SIMPLE METALS | - |
dc.subject.keywordPlus | COLLECTIVE STATES | - |
dc.subject.keywordPlus | RESONANCE | - |
dc.subject.keywordPlus | LITHIUM | - |
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