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dc.contributor.authorReshak, Ali H.
dc.contributor.authorAuluck, S.
dc.contributor.authorKityk, I. V.
dc.contributor.authorYarub K.A, Al-Douri
dc.contributor.authorKhenata, R.
dc.contributor.authorBouhemadou, A.
dc.date.accessioned2009-07-16T07:58:52Z
dc.date.available2009-07-16T07:58:52Z
dc.date.issued2009
dc.identifier.citationApplied Physics A : Materials Science and Processing, vol.94 (2), February 2009, pages 315-320.en_US
dc.identifier.issn0947-8396 (Print)
dc.identifier.issn1432-0630 (Online)
dc.identifier.urihttp://www.springerlink.com/content/mqq44r6183562kn2/
dc.identifier.urihttp://dspace.unimap.edu.my/123456789/6457
dc.descriptionLink to publisher's homepage at http://www.springerlink.com/content/mqq44r6183562kn2/en_US
dc.description.abstractWe report theoretical calculations of the band structure and density of states for orthorhombic LiGaS2 (LGS) and LiGaSe2 (LGSe). These calculations are based on the full potential linear augmented plane wave (FP-LAPW) method within a framework of density functional theory. Our calculations show that these crystals have similar band structures. The valence band maximum (VBM) and the conduction band minimum (CBM) are located at Γ, resulting in a direct energy band gap. The VBM is dominated by S/Se-p and Li-p states, while the CBM is dominated by Ga-s, S/Se-p and small contributions of Li-p and Ga-p. From the partial density of states we find that Li-p hybridizes with Li-s below the Fermi energy (E F), while Li-s/p hybridizes with Ga-p below and above E F. Also, we note that S/Se-p hybridizes with Ga-s below and above E F.en_US
dc.language.isoenen_US
dc.publisherSpringer Berlin/Heidelbergen_US
dc.subjectCrystallographyen_US
dc.subjectTellurium compoundsen_US
dc.subjectCrystalsen_US
dc.subjectSulfuren_US
dc.subjectLithiumen_US
dc.titleElectronic properties of orthorhombic LiGaS2 and LiGaSe 2en_US
dc.typeWorking Paperen_US


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