Electronic structures inVO 2 susing the periodic polarizable point-ion shell model and DV-Xα method
Author(s) -
Hiroshi Nakatsugawa,
E. Iguchi
Publication year - 1997
Publication title -
physical review. b, condensed matter
Language(s) - English
Resource type - Journals
eISSN - 1095-3795
pISSN - 0163-1829
DOI - 10.1103/physrevb.55.2157
Subject(s) - physics , hamiltonian (control theory) , electron , condensed matter physics , electronic correlation , crystallography , quantum mechanics , chemistry , mathematical optimization , mathematics
Electronic structures in the metallic $VO_{2}$ above the metal-insulator (MI) transition temperature of $T_{c}$ and the insulation phase below $T_{c}$ have been investigated using the combination of the three-dimensional periodic shell model and the discrete-variational (DV)-Xα cluster method. Besides the correlation effect for $d_{1}$ electrons, the Hamiltonian in the insulating phase includes the Anderson's attractive potentional due to the electron-phonon interactions which stabilize the three-dimensional periodic distribution of $V^{4+}-V^{4+}$ dimers.The shell model estimates the electron-phonon coupling constant and provides direct theoretical evidence that the dimers are stable in the low-temperature phase. The (DV)-Xα cluster method calculates the electron energie in $[V_{2}O_{10}] ^{-12}$ clusters and the values for the intersite repulsive nearest-neighbor d-d Coulombic interaction which quantifies the correlation effect for $d_{∥}$ electrons. The electron-phonon interaction effect and the correlation effect for d electrons are found to split $d_{∥}$ band into the empty upper and the occupied lower Hubbard bands and also to result in an obvious energy gap between these bands in the insulating phase. In the metallic phase, the nonresolved d band overlaps the $π_{*}$ band and they construct a partially filled conduction band.These calculations explain well the MI transition in $VO_{2}$ and, in particular, the electron-phonon interation assessed by periodic shell model is an indispensable contribution in the stabilization of the insulating phase
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