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An Electronic Model for CoO₂ layer based systems: Chiral RVB metal and Superconductivity

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arxiv cond-mat/0303649 v2 pith:2B3K5SOQ submitted 2003-03-31 cond-mat.str-el cond-mat.mtrl-scicond-mat.supr-con

An Electronic Model for CoO₂ layer based systems: Chiral RVB metal and Superconductivity

classification cond-mat.str-el cond-mat.mtrl-scicond-mat.supr-con
keywords chiralmodelsuperconductivitydeltalayermetalmottstate
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Takada et al. have reported superconductivity in layered $Na__x CoO_2.yH_2O$ ($T_c \approx5 K$) and more recently Wen et al. in $A_xCoO_{2+\delta}$ ($A = Na,K$)(\tc$\approx~31 K$). We model a reference neutral \cob layer as an orbitally non-degenerate spin-\half antiferromagnetic Mott insulator on a triangular lattice and $Na__x CoO_2.yH_2O$ and $A_xCoO_{2+\delta}$ as electron doped Mott insulators described by a t-J model. It is suggested that at optimal doping chiral spin fluctuations enhanced by the dopant dynamics leads to a d-wave superconducting state. A chiral RVB metal, a PT violating state with condensed RVB gauge fields, with a possible weak ferromagnetism and low temperature p-wave superconductivity are also suggested at higher dopings.

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