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Professor Ansgar Liebsch
The Mott transition in transition metal oxides consisting of partially filled t2g bands, such as Ca2RuO4, LaTiO3 and V2O3, is studied using a recent extension of exact diagonalization dynamical mean field theory to multi-band materials [1,2]. In agreement with previous QMC studies of LaTiO3 [3] and V2O3 [4], it is shown that the crystal filed splitting between t2g subbands is greatly enhanced by local Coulomb interactions, giving rise to a filling or emptying of one subset of t2g bands and a Mott transition in the remaining half-filled subset. Accordingly, the excitation gap involves transitions between the filled t2g bands and the upper Hubbard band of the half-filled subset, or the lower Hubbard band of the half-filled subset and the remaining emtpy t2g bands. The Mott transition in these materials may therefore be described as a hybrid Mott band metal insulator transition. [1] A. Perroni, H. Ishida, A. Liebsch, PRB (2007)
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