Covalent bonding and the nature of band gaps in some half-Heusler compounds

Half-Heusler compounds XYZ, also called semi-Heusler compounds, crystallize in the C1b MgAgAs structure, in the space group . 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 that the most appropriate description of these compounds from the viewpoint of electronic structures is one of a YZ zinc blende lattice stuffed by the 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 Ti4+ + (CoSb)4−; the latter unit is isoelectronic and isostructural with zinc-blende GaSb. For both the 8- and the 18-electron compounds, when X is fixed as some electropositive cation, the computed band gap varies approximately as the difference in Pauling electronegativities of Y and Z. What is particularly exciting is that this simple idea of a covalently bonded YZ lattice can also be extended to the very important magnetic half-Heusler phases; we describe these as valence compounds, i.e. possessing a band gap at the Fermi energy albeit only in one spin direction. The local moment in these magnetic compounds resides on the X site.

[1]  Axel D. Becke,et al.  A Simple Measure of Electron Localization in Atomic and Molecular-Systems , 1990 .

[2]  I. Dasgupta,et al.  Electronic structure and magnetism in half-Heusler compounds , 2003 .

[3]  H. Nowotny,et al.  Die Verbindungen LiMgP, LiZnP und LiZnAs , 1950 .

[4]  Allen,et al.  Band gaps and electronic structure of transition-metal compounds. , 1985, Physical review letters.

[5]  A. Savin,et al.  Classification of chemical bonds based on topological analysis of electron localization functions , 1994, Nature.

[6]  Christensen Electronic structure and bonding in ternary Zintl phases: LiAlSi. , 1985, Physical review. B, Condensed matter.

[7]  Band gap and stability in the ternary intermetallic compounds NiSnM (M=Ti,Zr,Hf): A first-principles study. , 1994, Physical review. B, Condensed matter.

[8]  K. Kushida,et al.  Growth and band gap of the filled tetrahedral semiconductor LiMgN , 1999 .

[9]  M. A. Kouacou,et al.  Properties on request in semi-Heusler phases , 1997 .

[10]  Richard Dronskowski,et al.  Crystal orbital Hamilton populations (COHP): energy-resolved visualization of chemical bonding in solids based on density-functional calculations , 1993 .

[11]  K.H.J. Buschow,et al.  New Class of Materials: Half-Metallic Ferromagnets , 1983 .

[12]  K.H.J. Buschow,et al.  Magneto-optical properties of metallic ferromagnetic materials , 1983 .

[13]  Bonding in MgSi and Al-Mg-Si compounds relevant to Al-Mg-Si alloys , 2003, cond-mat/0302027.

[14]  M. Whangbo,et al.  Study of the 18-electron band gap and ferromagnetism in semi-Heusler compounds by non-spin-polarized electronic band structure calculations , 2000 .

[15]  J. C. Phillips,et al.  Spectroscopic Analysis of Cohesive Energies and Heats of Formation of Tetrahedrally Coordinated Semiconductors , 1970 .

[16]  O. K. Andersen,et al.  Calculated electronic structure of the sandwichd1 metals LaI2 and CeI2: Application of new LMTO techniques , 1995 .

[17]  S. Jobic,et al.  Occurrence and characterization of anionic bondings in transition metal dichalcogenides , 1992 .

[18]  Jürgen Kübler,et al.  Formation and coupling of magnetic moments in Heusler alloys , 1983 .

[19]  O. K. Andersen,et al.  Linear methods in band theory , 1975 .

[20]  S. Kauzlarich,et al.  Structure and properties of the transition-metal zintl compounds A14MnPn11 (A = Ca, Sr, Ba; Pn = As, Sb) , 1994 .

[21]  P. H. Dederichs,et al.  Origin and properties of the gap in the half-ferromagnetic Heusler alloys , 2002 .

[22]  S. Kauzlarich,et al.  Structure and properties of the transition-metal zintl compounds: A14MnBi11 (A = Ca, Sr, Ba) , 1992 .

[23]  Wood,et al.  Electronic structure of filled tetrahedral semiconductors. , 1985, Physical review. B, Condensed matter.

[24]  T. Hughbanks,et al.  Stabilization of Metal-Rich Compounds by Polar-Intermetallic Bonding. Synthesis, Structure, and Bonding in Hf5MTe3 (M = Fe, Co) , 1995 .

[25]  E. C. Stoner,et al.  Collective Electron Ferromagnetism , 1938 .

[26]  L. Brewer,et al.  Erratum to: Transition metal alloys of extraordinary stability; An example of generalized Lewis-acid-base interactions in metallic systems , 1973 .

[27]  Elisabeth Sjöstedt,et al.  Efficient linearization of the augmented plane-wave method , 2001 .

[28]  R. Juza,et al.  Die ternären Nitride LiMgN und LiZnN. 16. Mitteilung über Metallamide und Metallnitride , 1948 .

[29]  Pierre Villars,et al.  Pearson's handbook of crystallographic data for intermetallic phases , 1985 .

[30]  R. Hoffmann,et al.  Metal-metal interactions, a pairing distortion, and S-lined channels in the M2Ta9S6 structure , 1988 .

[31]  J. Toboła,et al.  Electronic phase diagram of the XTZ (X=Fe, Co, Ni; T=Ti, V, Zr, Nb, Mn; Z=Sn, Sb) semi-Heusler compounds , 2000 .