6533b7dafe1ef96bd126f65e
RESEARCH PRODUCT
Covalent bonding and the nature of band gaps in some half-Heusler compounds
Claudia FelserRam SeshadriHem C. Kandpalsubject
Materials scienceAcoustics and UltrasonicsBand gapFOS: Physical sciencesIonic bonding02 engineering and technology01 natural sciencesIonElectronegativityCondensed Matter::Materials ScienceCondensed Matter - Strongly Correlated ElectronsLattice (order)0103 physical sciencesIsostructural010306 general physicsCondensed Matter - Materials ScienceValence (chemistry)Strongly Correlated Electrons (cond-mat.str-el)Materials Science (cond-mat.mtrl-sci)Fermi energy021001 nanoscience & nanotechnologyCondensed Matter Physics3. Good healthSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCrystallographyCondensed Matter::Strongly Correlated Electrons0210 nano-technologydescription
Half-Heusler compounds \textit{XYZ}, also called semi-Heusler compounds, crystallize in the MgAgAs structure, in the space group $F\bar43m$. We report a systematic examination of band gaps and the nature (covalent or ionic) of bonding in semiconducting 8- and 18- electron half-Heusler compounds through first-principles density functional calculations. We find the most appropriate description of these compounds from the viewpoint of electronic structures is one of a \textit{YZ} zinc blende lattice stuffed by the \textit{X} ion. Simple valence rules are obeyed for bonding in the 8-electron compound. For example, LiMgN can be written Li$^+$ + (MgN)$^-$, and (MgN)$^-$, which is isoelectronic with (SiSi), forms a zinc blende lattice. The 18-electron compounds can similarly be considered as obeying valence rules. A semiconductor such as TiCoSb can be written Ti$^{4+}$ + (CoSb)$^{4-}$; the latter unit is isoelectronic and isostructural with zinc-blende GaSb. For both the 8- and 18-electron compounds, when \textit{X} is fixed as some electropositive cation, the computed band gap varies approximately as the difference in Pauling electronegativities of \textit{Y} and \textit{Z}. What is particularly exciting is that this simple idea of a covalently bonded \textit{YZ} lattice can also be extended to the very important \textit{magnetic} half-Heusler phases; we describe these as valence compounds \textit{ie.} possessing a band gap at the Fermi energy albeit only in one spin direction. The \textit{local} moment in these magnetic compounds resides on the \textit{X} site.
year | journal | country | edition | language |
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2005-09-18 |