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arXiv · 0711.1702

Predominant Magnetic States in Hubbard Model on Anisotropic Triangular Lattices

Tsutomu Watanabe·Hisatoshi Yokoyama·Yukio Tanaka·Jun-ichiro Inoue
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Abstract

Using an optimization variational Monte Carlo method, we study the half-filled-band Hubbard model on anisotropic triangular lattices, as a continuation of the preceding study [J. Phys. Soc. Jpn 75, 074707 (2006)]. We introduce two new trial states: (i) A coexisting state of (π,π)-antiferromagnetic (AF) and a d-wave singlet gaps, in which we allow for a band renormalization effect, and (ii) a state with an AF order of 120^\circ spin structure. In both states, a first-order metal-to-insulator transition occurs at smaller U/t than that of the pure d-wave state. In insulating regimes, magnetic orders always exist; an ordinary (π,π)-AF order survives up to t'/t\sim 0.9 (U/t=12), and a 120^\circ-AF order becomes dominant for t'/t \gsim 0.9. The regimes of the robust superconductor and of the nonmagnetic insulator the preceding study proposed give way to these magnetic domains.

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Tsutomu Watanabe, Hisatoshi Yokoyama, Yukio Tanaka, Jun-ichiro Inoue. 2008-06-30. Predominant Magnetic States in Hubbard Model on Anisotropic Triangular Lattices. https://doi.org/10.1016/j.jmmm.2006.10.106

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