Show simple item record

dc.contributor.authorAli Hussain, Reshak, Prof. Dr.
dc.contributor.authorLakshminarayana, Gandham
dc.contributor.authorEbothe, Jean
dc.contributor.authorFedorchuk, Anatolii O.
dc.contributor.authorFedyna, M.F.
dc.contributor.authorKamarudin, Hussin, Brig. Jen. Dato' Prof. Dr.
dc.contributor.authorMandracci, P.
dc.contributor.authorAuluck, Sushil, Dr.
dc.date.accessioned2014-03-11T03:47:56Z
dc.date.available2014-03-11T03:47:56Z
dc.date.issued2013-04
dc.identifier.citationJournal of Alloys and Compounds, vol.556, 2013, pages 259-265en_US
dc.identifier.issn0925-8388
dc.identifier.urihttp://dspace.unimap.edu.my:80/dspace/handle/123456789/32496
dc.descriptionLink to publisher's homepage at http://www.elsevier.com/en_US
dc.description.abstractUsing FP-LAPW Method we have performed calculations of the band structure of the ZrGa₂ and ZrGa₃ crystals. The all-electron full potential linearized augmented plane wave method was used to solve the Kohn Sham DFT equations. We have explored different approximations using three kinds of exchange-correlation potentials on the electronic structure and we concluded that there is insignificant influence on the band structure and the density of states. It is clear that there exists a difference in the band dispersion with one move from ZrGa₂ to ZrGa₃ that is attributed to the fact that ZrGa₂ has four formula per unit cell (Z = 4) while ZrGa₃ has two formula per unit cell (Z = 2). Despite some similarity in the crystallochemistry of ZrGa₂ to ZrGa₃ some differences are observed in the band structure dispersion. There is a strong hybridization between the states. The interaction of charges between Zr and Ga atoms is due to the strong hybridization, and the covalent bond arises due to the degree of hybridization. Hence, there is a strong covalent bonding between these atoms. We have obtained a space electron charge density distribution in the average unit cell by calculations of the electron charge density distribution. The space electronic charge density contour distribution is illustrated in (1 0 0) and (1 1 0) planes.en_US
dc.language.isoenen_US
dc.publisherElsevieren_US
dc.subjectInorganic materialsen_US
dc.subjectCrystal growthen_US
dc.subjectElectronic band structureen_US
dc.subjectX-ray diffractionen_US
dc.titleBand structure, density of states, and crystal chemistry of ZrGa₂ and ZrGa₃ single crystalsen_US
dc.typeArticleen_US
dc.identifier.urlhttp://www.sciencedirect.com/science/article/pii/S092583881202381X
dc.identifier.urlhttp://dx.doi.org/10.1016/j.jallcom.2012.12.138
dc.contributor.urlmaalidph@yahoo.co.uken_US
dc.contributor.urlglnphysics@rediffmail.comen_US


Files in this item

Thumbnail

This item appears in the following Collection(s)

Show simple item record