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(Color online) (a) Phase diagram of the isotropic case with J ± = J p = J z = U/4 in U/t-α plane. (b) The Mott transitions in both orbitals at J ± = J p = J z = U/12 and J ± = J p = J z = U/6 as a function of U/t at α = 0. Here α = t a y /t a x and t b y /t b x = 1. 

(Color online) (a) Phase diagram of the isotropic case with J ± = J p = J z = U/4 in U/t-α plane. (b) The Mott transitions in both orbitals at J ± = J p = J z = U/12 and J ± = J p = J z = U/6 as a function of U/t at α = 0. Here α = t a y /t a x and t b y /t b x = 1. 

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By applying dynamical mean-field theory in combination with exact diagonalization at zero temperature to a half-filled Hubbard model with two orbitals having distinct noninteracting densities of states, we show that an orbital selective Mott transition (OSMT) will take place even without crystal field splitting, differences in bandwidth and orbital...

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