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Band structure effects on the superconductivity in Hubbard models

机译:能带结构对哈伯德模型超导性的影响

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We study the influence of the band structure on the symmetry and superconducting transition temperature in the (solvable) weak-coupling limit of the repulsive Hubbard model. Among other results we find that (1) as a function of increasing nematicity, starting from the square-lattice (zero nematicity) limit where a nodal d-wave state is strongly preferred, there is a smooth evolution to the quasi-ID limit, where a striking near-degeneracy is found between a p-wave- and a d-wave-type paired states with accidental nodes on the quasi-one-dimensional Fermi surfaces-a situation that may be relevant to the Bechgaard salts. (2) In a bilayer system, we find aphase transition as a function of increasing bilayer coupling from a d-wave to an s_±-wave state reminiscent of the iron-based superconductors. (3) When an antinodal gap is produced by charge-density-wave order, not only is the pairing scale reduced, but the symmetry of the pairs switches from d_(x~2-y~2) to d_(xy) in the context of the cuprates, this suggests that were the pseudogap entirely due to a competing CDW order, this would likely cause a corresponding symmetry change of the superconducting order (which is not seen in experiment).
机译:我们在排斥哈伯德模型的(可解)弱耦合极限中研究了能带结构对对称性和超导转变温度的影响。在其他结果中,我们发现(1)作为向列性增加的函数,从强烈优先考虑节点d波状态的方格(零向列性)极限开始,到准ID极限有一个平滑的演化,在准一维费米表面上有偶发节点的p波和d波型配对状态之间发现了惊人的近简并列现象,这种情况可能与Bechgaard盐有关。 (2)在双层系统中,我们发现相变是从d波到s_±波状态的双层耦合增加的函数,让人联想到铁基超导体。 (3)当电荷密度波阶产生反节点间隙时,不仅配对比例减小,而且配对的对称性从d_(x〜2-y〜2)切换为d_(xy)。在铜酸盐的背景下,这表明完全是由于竞争的CDW阶造成的伪间隙,这可能会导致超导阶的相应对称性变化(在实验中未见)。

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  • 来源
    《Physical review》 |2013年第6期|064505.1-064505.14|共14页
  • 作者单位

    Department of Physics, Stanford University, Stanford, California 94305, USA;

    Institut de Theorie des Phenomenes Physiques, Ecole Polytechnique Federate de Lausanne (EPFL), CH-1015 Lausanne, Switzerland,Institute for Theoretical Physics and Astrophysics, University of Wuerzburg, D 97074 Wuerzburg, Germany;

    Department of Physics, Stanford University, Stanford, California 94305, USA;

    Department of Physics, Stanford University, Stanford, California 94305, USA;

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