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Browsing by Author "Bulla, R."

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    Dynamical mean-field theory and its applications to real materials
    (Physical Soc Japan, 2005)
    Vollhardt, D.
    ;
    Held, Kathrin
    ;
    Keller, G.
    ;
    Bulla, R.
    ;
    Pruschke, T.
    ;
    Nekrasov, I. A.
    ;
    Anisimov, V. I.
    Dynamical mean-field theory (DMFT) is a non-perturbative technique for the investigation of correlated electron systems. Its combination with the local density approximation (LDA) has recently led to a material-specific computational scheme for the ab initio investigation of correlated electron materials. The set-up of this approach and its application to materials such as (Sr,Ca)VO3, V2O3, and Cerium is discussed. The calculated spectra are compared with the spectroscopically measured electronic excitation spectra. The surprising similarity between the spectra of the single-impurity Anderson model and of correlated bulk materials is also addressed.
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    Hund's coupling and the metal-insulator transition in the two-band Hubbard model
    (Springer, 2005)
    Pruschke, T.
    ;
    Bulla, R.
    The Mott-Hubbard metal-insulator transition is investigated in a two-band Hubbard model within dynamical mean-field theory. To this end, we use a suitable extension of Wilson's numerical renormalization group for the solution of the effective two-band single-impurity Anderson model. This method is non-perturbative and, in particular, allows to take into account the full exchange part of the Hund's rule coupling between the two orbitals. We discuss in detail the influence of the various Coulomb interactions on thermodynamic and dynamic properties, for both the impurity and the lattice model. The exchange part of the Hund's rule coupling turns out to play an important role for the physics of the two-band Hubbard model and for the nature of the Mott-transition.
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    Phase diagram of the frustrated Hubbard model
    (American Physical Soc, 2004)
    Zitzler, R.
    ;
    Tong, N. H.
    ;
    Pruschke, T.
    ;
    Bulla, R.
    The Mott-Hubbard metal-insulator transition in the paramagnetic phase of the one-band Hubbard model has long been used to describe similar features in real materials like V2O3. In this Letter we investigate the antiferromagnetic phase of this model with frustration. At T=0 we find a first-order transition from a paramagnetic metal to an antiferromagnetic insulator. We show that even in the presence of strong magnetic frustration, the paramagnetic metal-insulator transition is hidden inside an extended antiferromagnetic region. This raises the question of whether the one-band Hubbard model with frustration is sufficient to describe the phase diagram of V2O3 or similar transition metal oxides even qualitatively.

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