Tight-Binding Superconducting Phases in the Unconventional Compounds Strontium-Substituted Lanthanum Cuprate and Strontium Ruthenate

Pedro L. Contreras E., Dianela Osorio, E. Beliayev
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引用次数: 4

Abstract

: We use the idea of the Wigner probability distribution (WPD) in a reduced scattering phase space (RPS) for the elastic scattering cross-section, with the help of a Tight-Binding (TB) numerical procedure allowing us to consider the anisotropic quantum effects, to phenomenologically predict several phases in these two novel unconventional superconductors. Unlike our previous works with pieces of evidences that these two compounds are in the unitary strong scattering regime and that superconductivity is suppressed by the atoms of strontium in both materials, several phases are built. In the case of the strontium-substituted lanthanum cuprate, it was found three phases from one family of Wigner probabilistic distributions, one corresponding to the antiferromagnetic compound La 2 CuO 4 another one which consists of a coalescing metallic phase for very lightly doped La 2-x Sr x CuO 4 , and finally a strong self-consistent dependent strange metal phase with optimal levels of doping. In the case of a triplet superconductor strontium ruthenate, three phases can be differentiated from two families of Wigner distribution probabilities, one family of WDP with point nodes where Cooper pairs and dressed scattered normal quasiparticles are mixed for the whole range of frequencies and which correspond to a FS γ-flat-sheet in the ground metallic state, and two phases from another WPD family, where, in one of then, the Miyake-Narikiyo quasinodal tiny gap model allows the unique presence of Cooper pairs in a tiny interval of frequencies near the superconducting transition T C , the other phase corresponds to the mixed phase with Cooper pairs and dressed by stoichiometric strontium non-magnetic atoms, where strong self-consistent effects are noticeable. This approach allows comparing experimental results for samples in both compounds with numerical analysis studies.
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非常规化合物锶取代铜酸镧和钌酸锶中的紧密结合超导相
我们利用维格纳概率分布(WPD)在简化散射相空间(RPS)中的思想作为弹性散射截面,借助紧束缚(TB)数值程序,允许我们考虑各向异性量子效应,对这两种新型非常规超导体中的几个相进行了现象学预测。不像我们之前的工作,这两种化合物都处于单一的强散射状态,并且超导性被两种材料中的锶原子抑制。在锶取代铜酸镧的情况下,发现了来自一个Wigner概率分布族的三个相,一个对应于反铁磁化合物la2cuo4,另一个由极轻掺杂的la2 -x Sr x cuo4的聚结金属相组成,最后是一个具有最佳掺杂水平的强自一致性依赖的奇怪金属相。在三重态超导体钌酸锶的情况下,可以从两个Wigner分布概率族中区分出三个相,一个WDP族具有点节点,其中Cooper对和被修饰的散射正常准粒子在整个频率范围内混合,对应于基态的FS γ-平板,另一个WPD族的两个相,其中一个,Miyake-Narikiyo准节点微小间隙模型允许在超导跃迁tc附近的微小频率区间内独特地存在库珀对,另一个相对应于库珀对的混合相,并由化学计量的锶非磁性原子包裹,其中强自一致效应是明显的。这种方法允许将两种化合物样品的实验结果与数值分析研究进行比较。
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