Abstract

We use an efficient general hybridization-expansion continuous-time quantum Monte Carlo impurity solver (Krylov approach) to study orbital and spin ordering phenomena in strongly correlated systems within the local-density approximation plus dynamical mean-field theory approach. This allows us to include often-neglected interaction terms, to study models with large basis sets, to consider crystals with low-symmetry distortions, and to reach the very low experimental temperatures. We use this solver to study ordering phenomena in a selection of exemplary low-symmetry transition-metal oxides. For the rare-earth manganites, we show that including spin-flip and pair-hopping terms does not affect the Kugel-Khomskii orbital-order melting transition. For LaMnO${}_{3}$, we find that the commonly used two-band model with classical ${t}_{2g}$ spin gives a good description of the ${e}_{g}$ electrons when compared with the full five-orbital Hubbard model. Surprisingly not only the occupied orbital but also the ${e}_{g}$ spectral matrix is well reproduced. For the ${d}^{1}$ perovskites CaVO${}_{3}$ and YTiO${}_{3}$ we show that spin-flip and pair-hopping terms only weakly affect orbital fluctuations. Moreover, for the Mott insulator YTiO${}_{3}$ we can study the ferromagnetic polarization to very low temperatures, finding a transition temperature in remarkably good agreement with experiments.

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