NaCoO in the x -> 0 Regime: Coupling of Structure and Correlation effects
arXiv:cond-mat/0505606 · doi:10.1103/PhysRevB.72.115110
Abstract
The study of the strength of correlations in NaCoO is extended to the x=0 end of the phase diagram where Mott insulating behavior has been widely anticipated. Inclusion of correlation as modeled by the LDA+U approach leads to a Mott transition in the subband if U is no less than U=2.5 eV. Thus U smaller than U is required to model the metallic, nonmagnetic CoO compound reported by Tarascon and coworkers. The orbital-selective Mott transition of the state, which is essentially degenerate with the states, occurs because of the slightly wider bandwidth of the bands. The metal-insulator transition is found to be strongly coupled to the Co-O bond length, due to associated changes in the bandwidth, but the largest effects occur only at a reduced oxygen height that lies below the equilibrium position.
8 pages with 9 embedded figures
References in corpus (5)
- Ferromagnetic fluctuation and possible triplet superconductivity in Na_xCoO_2*yH_2O: Fluctuation-exchange study of multi-orbital Hubbard model
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Cited by in corpus (5)
- Synthesis and properties of CoO2, the x = 0 end member of the LixCoO2 and NaxCoO2 systems
- Electronic Correlations in CoO2, the Parent Compound of Triangular Cobaltates
- Elliptical hole pockets in the Fermi surfaces of unhydrated and hydrated sodium cobalt oxides
- Electrochemical synthesis and properties of CoO2, the x = 0 phase of the AxCoO2 systems (A = Li, Na)
- Disproportionation and Critical Interaction Strength in NaCoO: Concentration Dependence