Large time effective kinetics $β$-function for quantum (2+p)-spin glass

Vincent Lahoche, Dine Ousmane Samary, Parham Radpay
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Abstract

This paper examines the quantum $(2+p)$-spin dynamics of a $N$-vector $\textbf{x}\in \mathbb{R}^N$ through the lens of renormalization group (RG) theory. The RG is based on a coarse-graining over the eigenvalues of matrix-like disorder, viewed as an effective kinetic whose eigenvalue distribution undergoes a deterministic law in the large $N$ limit. We focus our investigation on perturbation theory and vertex expansion for effective average action, which proves more amenable than standard nonperturbative approaches due to the distinct non-local temporal and replicative structures that emerge in the effective interactions following disorder integration. Our work entails the formulation of rules to address these non-localities within the framework of perturbation theory, culminating in the derivation of one-loop $\beta$-functions. Our explicit calculations focus on the cases $p=3$, $p=\infty$, and additional analytic material is given in the appendix.
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量子(2+p)-自旋玻璃的大时间有效动力学β$函数
本文通过重正化群(RG)理论的视角,研究了N$矢量$textbf{x}\\mathbb{R}^N$中的量子$(2+p)$自旋动力学。重正化群理论基于对类似矩阵的无序特征值的粗粒度化,它被视为一种有效动力学,其特征值分布在大 $N$ 极限下经历了一个确定性规律。我们的研究重点是有效平均作用的扰动理论和顶点展开,这比标准的非扰动方法更适用于无序整合后有效相互作用中出现的独特非局部时间和复制结构。我们的工作需要在扰动理论的框架内制定规则来解决这些非局部性问题,最终推导出单环的(beta)函数。我们的显式计算集中于 $p=3$,$p=\infty$的情况,附录中给出了额外的分析材料。
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