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Interplay of Pomeranchuk instability and superconductivity in the two-dimensional repulsive Hubbard model

机译:Pomeranchuk不稳定性和超导中的相互作用在二维排斥喧嚣模型中

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Interplay of Pomeranchuk instability (spontaneous symmetry breaking of the Fermi surface) and d-wave superconductivity is studied for the repulsive Hubbard model on the square lattice with the dynamical mean-field theory combined with the fluctuation exchange approximation (FLEX+DMFT). We show that the fourfold symmetric Fermi surface becomes unstable against a spontaneous distortion into twofold near the van Hove filling, where the symmetry of superconductivity coexisting with the Pomeranchuk-distorted Fermi surface is modified from the d-wave pairing to the (d + s) wave. By systematically shifting the position of van Hove filling with varied second- and third-neighbor hoppings, we find that the transition temperature T~(PI)_c for the Pomeranchuk instability is more sensitively affected by the position of van Hove filling than the superconducting T~(SC)_c . This implies that the filling region for strong Pomeranchuk instability and that for the T~(SC)_c dome can be separated, and that Pomeranchuk instability can appear even if the peak of T~(PI)_c is lower than the peak of T~(SC)_c . An interesting finding is that the Fermi surface distortion can enhance the superconducting T~(SC)_c in the overdoped regime, which is explained with a perturbational picture for small distortions.
机译:利用动态平均场理论与波动交换近似(Flex + DMFT)相结合的方形格子上的排斥屋格模型研究了Pomeranchuk的不稳定性(Fermi表面的自发对称断裂)和D波超导。我们表明,四倍对称的费米表面抵抗在van Hove填充附近的双重变形中的自发性畸变,其中超导电性与Pomeranchuk扭曲的费米表面的对称性从D波配对改变为(D + S)海浪。通过系统地使Van Hove填充用不同的第二和第三邻居跳纸的位置,我们发现Pomeranchuk不稳定性的过渡温度T〜(PI)_C比超导T的范围填充的位置更灵敏地影响〜(sc)_c。这意味着可以分离强烈的Pomeranchuk不稳定性的填充区域,并且可以分离用于T〜(SC)_C圆顶的填充区域,即使T〜(PI)_c的峰值低于T〜的峰值,也可以出现Pomeranchuk不稳定性(SC)_C。一个有趣的发现是,费米表面失真可以增强过掺杂的制度中的超导T〜(SC)_C,这将用扰动图像来解释用于小畸变。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2017年第8期|075109.1-075109.7|共7页
  • 作者单位

    Department of Physics University of Tokyo Hongo Tokyo 113-0033 Japan;

    RIKEN Center for Emergent Matter Science (CEMS) Wako 351-0198 Japan;

    Department of Physics University of Tokyo Hongo Tokyo 113-0033 Japan Electronics and Photonics Research Institute Advanced Industrial Science and Technology (AIST) Tsukuba Ibaraki 305-8568 Japan;

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