167 research outputs found

    Evaluation of Compensated Magnetism in La2_2VCuO6_6: Exploration of Charge States

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    We present an ab initio study of double perovskite La2_2VCuO6_6, which was one of the earliest compounds suggested as a potential compensated half-metal. Two charge and spin configurations close in energy have been identified. (i) The originally envisioned spin-compensated V4+^{4+}:d1^1/Cu2+^{2+}:d1^1 configuration is comprised of antialigned S=1/2 cations. This state is a spin-compensated half-metal for moderate values of U (the on-site Coulomb repulsion strength on the metal ions) and is insulating for larger values of U. (ii) An unanticipated non-magnetic solution V5+^{5+}:d0^0/Cu+^{+}:d10^{10} consists of an empty- and a full-shell ion, both spherically symmetric, that leads to a band insulator. This ionic band insulator is calculated to be the ground state at small and moderate values of U. The different distortions of the perovskite structure that occur for each state are central in determining the energy differences. Treating the Cu2+^{2+} Jahn-Teller distortion self-consistently is particularly important for the magnetic solution.Comment: 5 pages, 2 figures, 1 tabl

    Quantum Confinement Induced Molecular Mott Insulating State in La4_4Ni3_3O8_8

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    The recently synthesized layered nickelate La4_4Ni3_3O8_8, with its cuprate-like NiO2_2 layers, seemingly requires a Ni1 (d8d^8)+2Ni2 (d9d^9) charge order, together with strong correlation effects, to account for its insulating behavior. Using density functional methods including strong intra-atomic repulsion (Hubbard U), we obtain an insulating state via a new mechanism: {\it without charge order}, Mott insulating behavior arises based on quantum coupled, spin-aligned Ni2-Ni1-Ni2 dz2d_{z^2} states across the trilayer (rather than based on atomic states), with antiferromagnetic ordering within layers. The weak and frustrated magnetic coupling between cells may account for the small spin entropy that is removed at the N\'eel transition at 105 K and the lack of any diffraction peak at the N\'eel point.Comment: 4 pages, 3 figure
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