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Incommensurable state of a spin density wave and superconductivity in quasi-two-dimensional systems with an anisotropic energy spectrum

机译:具有各向异性能谱的准二维系统中自旋密度波和超导的不可估量状态

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We investigate phase transitions in quasi-two-dimensional systems with an anisotropic energy spectrum and a deviation from the half-filling of the energy band (μ ≠ 0). We demonstrate the possibility of the transition of an insulator into a half-metallic state when the nesting condition is violated because the parameter μ ≠ 0 and of taking the umklapp processes into account. We obtain the basic equations for the parameters of the superconducting (Δ) and magnetic (M) orders and determine the conditions for the emergence of superconductivity on the background of a spin-density-wave state and also for the coexistence of superconductivity and magnetism. We show that the transition of a magnetic system into a superconducting state as the parameter μ increases can be a first-order phase transition at low temperatures. We also obtain an expression for the heat capacity jump C_S-C_N at T = T_c, which depends on M and μ and differs essentially from the case of the Bardeen-Cooper-Schrieffer theory. We also consider the transformations related to the density of electron states of the relevant anisotropic system, which can undergo essential changes under pressure or doping.
机译:我们研究具有各向异性能谱并且偏离能带半填充(μ≠0)的准二维系统的相变。我们证明了当由于参数μ≠0而违反嵌套条件时,绝缘子过渡到半金属状态的可能性,并考虑了umklapp过程。我们获得了超导(Δ)和磁(M)阶参数的基本方程式,并确定了自旋密度波状态背景下超导出现的条件以及超导和磁并存的条件。我们表明,随着参数μ的增加,磁系统向超导状态的转变可以是低温下的一阶相变。我们还获得了在T = T_c时热容跳跃C_S-C_N的表达式,该表达式取决于M和μ,并且与Bardeen-Cooper-Schrieffer理论的情况本质上不同。我们还考虑了与相关各向异性系统电子态密度有关的变换,这些变换在压力或掺杂下可能发生本质变化。

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