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Unconventional superconductivity in low density electron systems and conventional superconductivity in hydrogen metallic alloys under pressure

机译:低密度电子系统中的非常规超导性   压力下氢金属合金的常规超导性

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摘要

In a short review-article we first discuss the results, which are mainlydevoted to the generalizations of the famous Kohn-Luttinger mechanism ofsuperconductivity in purely repulsive fermion systems at low electrondensities. In the context of repulsive-U Hubbard model and Shubin-Vonsovskymodel we consider briefly the superconducting phase diagrams and the symmetriesof the order parameter in novel strongly correlated electron systems includingidealized monolayer and bilayer graphene. We stress that purely repulsivefermion systems are mainly the subject of unconventional low-temperaturesuperconductivity. To get the high temperature superconductivity in cuprates(with T_C of the order of 100 K) we should proceed to the t-J model with theVan der Waals interaction potential and the competition between short-rangerepulsion and long-range attraction. Finally we stress that to describesuperconductivity in metallic hydrogen alloys under pressure (with T_C of theorder of 200 K) it is reasonable to reexamine more conventional mechanismsconnected with electron-phonon interaction. These mechanisms arise in theattractive-U Hubbard model with static onsite or intersite attractive potentialor in more realistic theories (which include retardation effects) such asMigdal-Eliashberg strong coupling theory or even Fermi-Bose mixture theory ofRanninger et al., and its generalizations.
机译:在简短的评论文章中,我们首先讨论了结果,这些结果主要用于推广在低电子密度的纯斥力费米子系统中著名的Kohn-Luttinger超导机理。在排斥-U Hubbard模型和Shubin-Vonsovsky模型的背景下,我们简要考虑了新型强相关电子系统(包括理想化的单层和双层石墨烯)中的超导相图和阶跃参数的对称性。我们强调,纯斥力铁氧体系统主要是非常规低温超导性的主题。为了获得以铜酸盐表示的高温超导性(T_C约为100 K),我们应该进入具有范德华相互作用势以及短程排斥与长程吸引之间竞争的t-J模型。最后,我们强调指出,为了描述金属氢合金在压力(T_C约为200 K)下的超导性,有必要重新研究与电子-声子相互作用有关的更常规的机理。这些机制出现在具有静态现场或场间诱人潜力的有吸引力的U Hubbard模型中,或者在更现实的理论(包括阻滞效应)中,例如Migdal-Eliashberg强耦合理论甚至Ranninger等人的Fermi-Bose混合理论,及其推广。

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    Kagan, Maxim Yu.;

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