TY - JOUR
T1 - Covalent bonding and bandgap formation in transition-metal aluminides: Di-aluminides of group VIII transition metals
AU - Krajci, Marian
AU - Hafner, Juergen
N1 - Zeitschrift: Journal of Physics Condensed Matter
DOI: 10.1088/0953-8984/14/23/309
Coden: JCOME
Affiliations: Institut für Materialphysik, Ctr. for Computational Mat. Science, Universität Wien, Sensengasse 8/12, A-1090 Wien, Austria
Adressen: Kraj?í, M.; Institut für Materialphysik; Ctr. for Computational Mat. Science; Universität Wien; Sensengasse 8/12 A-1090 Wien, Austria; email: [email protected]
Import aus Scopus: 2-s2.0-0037124581
22.10.2007: Datenanforderung 1935 (Import Sachbearbeiter)
22.10.2007: Datenanforderung 1936 (Import Sachbearbeiter)
PY - 2002
Y1 - 2002
N2 - In this paper we study the electronic structure, electron density distribution and bonding mechanism in transition-metal (TM) di-aluminides Al2TM formed by metals of group VIII (TM Fe, Ru, Os) and crystal structures of TM di-silicides C11b (MoSi2), C40 (CrSi2) and C54 (TiSi2). A peculiar feature of the electronic structure of these TM di-aluminides is the existence of a semiconducting gap at the Fermi level. A substitution of a 3d TM by 4d or 5d metal enhances the width of the gap. From the analysis of the charge-density distribution and the crystal-orbital overlap population we conclude that the bonding between atoms has strong covalent character. This is confirmed not only from the enhanced charge density halfway between atoms, but also by a clear bonding-antibonding splitting of the electronic states. Groups of bonding and antibonding states corresponding to a particular bonding configuration of atoms are separated by a gap. As such a gap is observed in all bonding configurations among atoms in the unit cell it results in a gap in the total density of states. The bandgap exists at a certain electron per atom ratio e/A≈4.67 and also occurs in TM di-aluminides of groups VII and IX. For group VIII TM di-aluminides the Fermi level falls just in the gap.
AB - In this paper we study the electronic structure, electron density distribution and bonding mechanism in transition-metal (TM) di-aluminides Al2TM formed by metals of group VIII (TM Fe, Ru, Os) and crystal structures of TM di-silicides C11b (MoSi2), C40 (CrSi2) and C54 (TiSi2). A peculiar feature of the electronic structure of these TM di-aluminides is the existence of a semiconducting gap at the Fermi level. A substitution of a 3d TM by 4d or 5d metal enhances the width of the gap. From the analysis of the charge-density distribution and the crystal-orbital overlap population we conclude that the bonding between atoms has strong covalent character. This is confirmed not only from the enhanced charge density halfway between atoms, but also by a clear bonding-antibonding splitting of the electronic states. Groups of bonding and antibonding states corresponding to a particular bonding configuration of atoms are separated by a gap. As such a gap is observed in all bonding configurations among atoms in the unit cell it results in a gap in the total density of states. The bandgap exists at a certain electron per atom ratio e/A≈4.67 and also occurs in TM di-aluminides of groups VII and IX. For group VIII TM di-aluminides the Fermi level falls just in the gap.
U2 - 10.1088/0953-8984/14/23/309
DO - 10.1088/0953-8984/14/23/309
M3 - Article
SN - 0953-8984
VL - 14
SP - 5755
EP - 5783
JO - Journal of Physics: Condensed Matter
JF - Journal of Physics: Condensed Matter
IS - 23
ER -