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dc.contributor.authorAli Hussain, Reshak, Prof. Dr.-
dc.contributor.authorSikander, Azam-
dc.contributor.authorZeyad A., Alahmed-
dc.contributor.authorJan Chyský-
dc.date.accessioned2014-03-14T08:25:30Z-
dc.date.available2014-03-14T08:25:30Z-
dc.date.issued2014-02-
dc.identifier.citationJournal of Magnetism and Magnetic Materials, vol.351, 2014, pages 98–103en_US
dc.identifier.issn0304-8853-
dc.identifier.urihttp://dspace.unimap.edu.my:80/dspace/handle/123456789/32756-
dc.descriptionLink to publisher's homepage at http://www.elsevier.comen_US
dc.description.abstractThe band structure, density of states, electronic charge density, Fermi surface and optical properties for B₈(Be₄₈)B₂ compound has been investigated in the support of density functional theory (DFT). The atomic positions of B₈(Be₄₈)B₂ compound were optimized by minimization of the forces acting on the atoms using the full potential linear augmented plane wave (FPLAPW) method. We have employed the local density approximation (LDA), generalized gradient approximation (GGA) and Engal-Vosko GGA (EVGGA) to indulgence the exchange correlation potential by solving Kohn–Sham equations. The result shows that the compound is metallic with sturdy hybridization near the Fermi energy level (EF). The density of states at Fermi energy, N(EF), is determined by the overlaping between B-p, B-s and Be-s states. This overlaping is strong enough indicating metallic origin with different values of N(EF). These values are 16.4, 16.27 and 14.89 states/eV, and the corresponding bare linear low-temperature electronic specific heat coefficient (γ) is found to be 2.84, 2.82 and 2.58 mJ/mol K² for EVGGA, GGA and LDA respectively. There exists a strong hybridization between B-s and B-p states, also between B-s and Be-p states around the Fermi level. The Fermi surface is composed of three sheets. These sheets consist of set of holes and electrons. The bonding features of the compounds are analyzed using the electronic charge density in the (101 and −101) crystallographic planes and also the analyzing of charge density shows covalent bonding between B and B. The linear optical properties are also deliberated and discussed in particulars.en_US
dc.language.isoenen_US
dc.publisherElsevier/NORTH-HOLLANDen_US
dc.subjectCeramicsen_US
dc.subjectMetalsen_US
dc.subjectElectronic structureen_US
dc.subjectFermi surfaceen_US
dc.subjectOptical propertiesen_US
dc.titleElectronic structure, Fermi surface and optical properties of metallic compound Be₈(B₄₈)B₂en_US
dc.typeArticleen_US
dc.identifier.urlhttp://www.sciencedirect.com/science/article/pii/S0304885313007191-
dc.identifier.urlhttp://dx.doi.org/10.1016/j.jmmm.2013.09.060-
dc.contributor.urlsikander.physicst@gmail.comen_US
dc.contributor.urlsikandar_hu@yahoo.comen_US
Appears in Collections:Center of Excellence for Geopolymer and Green Technology (CEGEOGTECH) (Articles)
School of Materials Engineering (Articles)

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