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Using Wannier-functions, a low-energy Hamiltonian is derived for orthorhombic transition-metal oxides. Electronic correlations are treated with a new implementation of dynamical mean-field theory for non-cubic systems. Good agreement with photoemission data is obtained. The interplay of correlation effects and cation covalency (GdFeO-type distortions) is found to suppress orbital fluctuations in LaTiO and even more in YTiO, and to favor the transition to the insulating state.

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