Insulating phase ofV2O3: An attempt at a realistic calculation

Abstract
The problem of the highly correlated electron gas V2 O3 consisting of a filled a1g and a quarterly full eg band is treated on the basis of a Hartree-Fock calculation with spin and orbit unrestriction. The values of the effective hopping integrals which include covalency effects (due to the overlap of the 2pπ orbitals of the oxygens with the 3d wave functions of the vanadium atoms) are assessed on the bases of available bandstructure calculations and experimental results measuring covalency contributions. For reasonable values of the Hubbard parameters Umm2 eV, Umn1.6 eV, and Jmn0.2 eV [the interatomic Coulomb repulsion of electrons on the same orbit (m, m) on different orbits (m, n) and the exchange integral Jmn] it is found that the observed spin structure of V2 O3 together with an antiferromagnetic orbital order gives the lowest Hartree-Fock ground-state energy amongst a large class of solutions which we considered and shows a gap in the density of states of the order of 0.2-0.3 eV. Since this gap appears already in the trigonal phase, we feel confident that the monoclinic distortion in the low-temperature phase is of magnetostrictive origin and not a primary cause of the metal-insulator transition. The peculiar value of 1.2μB per V atom as observed by neutron scattering is interpreted as a strongly covalency-enhanced moment on the V atom. The atomic limit value of 1μB due to one magnetic eg electron per V atom is reduced to 0.75μB in an itinerant picture. The covalency mechanism providing the extra 0.4μB is known as back-bonding effect and leads at the same time to a negative spin density on the oxygen ions which are therefore no longer diamagnetic. Negative O17 NMR shift in the insulating antiferromagnetic phase should be able to verify this conjecture.