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Antiferromagnetic Ising spin glass competing with BCS pairing interaction in a transverse field

机译:反铁磁Ising旋转玻璃与BCs配对竞争   横向场中的相互作用

摘要

The competition among spin glass (SG), antiferromagnetism (AF) and localpairing superconductivity (PAIR) is studied in a two-sublattice fermionic Isingspin glass model with a local BCS pairing interaction in the presence of anapplied magnetic transverse field $\Gamma$. In the present approach, spins indifferent sublattices interact with a Gaussian random coupling with anantiferromagnetic mean $J_0$ and standard deviation $J$. The problem isformulated in the path integral formalism in which spin operators arerepresented by bilinear combinations of Grassmann variables. The saddle-pointGrand Canonical potential is obtained within the static approximation and thereplica symmetric ansatz. The results are analysed in phase diagrams in whichthe AF and the SG phases can occur for small $g$ ($g$ is the strength of thelocal superconductor coupling written in units of $J$), while the PAIR phaseappears as unique solution for large $g$. However, there is a complex linetransition separating the PAIR phase from the others. It is second order athigh temperature that ends in a tricritical point. The quantum fluctuationsaffect deeply the transition lines and the tricritical point due to thepresence of $\Gamma$.
机译:在存在局部磁场CS \γ的情况下,在具有局部BCS配对相互作用的两子晶格铁离子伊辛斯平玻璃模型中研究了自旋玻璃(SG),反铁磁性(AF)和局部对超导(PAIR)之间的竞争。在本方法中,自旋无差异的亚晶格与具有反磁平均值$ J_0 $和标准偏差$ J $的高斯随机耦合相互作用。问题是在路径积分形式主义中提出的,其中自旋算子由格拉斯曼变量的双线性组合表示。在静态逼近和对称对称ansatz内获得了鞍点大正则势。在相图中分析结果,在相图中,AF和SG阶段可能发生在较小的$ g $情况下($ g $是以$ J $表示的本地超导体耦合的强度),而PAIR阶段则显示为较大的唯一解决方案$ g $。但是,有一个复杂的线路过渡将PAIR相与其他相分离。在高温下的二阶终止于三临界点。由于存在\\ Gamma $,量子波动会深深影响过渡线和三临界点。

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