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      Charge and magnetic order in two-orbital double-exchange model for manganites

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          Abstract

          Phase diagram of half-doped perovskite manganites is studied within the extended double-exchange model. To demonstrate the role of orbital degrees of freedom both one- and two-orbital models are examined. A rich phase diagram is obtained in the mean-field theory at zero temperature as a function of J (antiferromagnetic (AFM) superexchange interaction) and V (intersite Coulomb repulsion). For the one-orbital model a charge-ordered (CO) state appears at any value of V with different types of magnetic order which changes with increasing J from ferromagnetic (F) to AFM ones of the types A, C and G. The orbital degeneracy results in appearance of a new CE-type spin order that is favorable due to opening of the "dimerization" gap at the Fermi surface. In addition, the CO state appears only for V>V_c for F and CE states while C-type AFM state disappears and A-type AFM state is observed only at small values of V as a charge disordered one. The relevance of our results to the experimental data are dicussed.

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          A First-Order Phase Transition Induced by a Magnetic Field

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            Collapse of a charge-ordered state under a magnetic field in Pr1/2Sr1/2MnO3.

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              Simultaneous Structural, Magnetic, and Electronic Transitions inLa1−xCaxMnO3withx=0.25 and 0.50

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                Author and article information

                Journal
                25 October 1999
                2000-04-08
                Article
                10.1103/PhysRevB.62.372
                cond-mat/9910391
                c979697d-22da-406c-a058-e1a30eb30bc7
                History
                Custom metadata
                Phys. Rev. B 62, 372 (2000)
                Contents is slightly modified. (To be published in Phys. Rev B1 01Jul.00)
                cond-mat.str-el

                Condensed matter
                Condensed matter

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