Critical edge behavior in the singularly perturbed Pollaczek–Jacobi type unitary ensemble

Zhaoyu Wang, E. Fan
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引用次数: 5

Abstract

In this paper, we study the strong asymptotic for the orthogonal polynomials and universality associated with singularly perturbed Pollaczek-Jacobi type weight $$w_{p_J2}(x,t)=e^{-\frac{t}{x(1-x)}}x^\alpha(1-x)^\beta, $$ where $t \ge 0$, $\alpha >0$, $\beta >0$ and $x \in [0,1].$ Our main results obtained here include two aspects: { I. Strong asymptotics:} We obtain the strong asymptotic expansions for the monic Pollaczek-Jacobi type orthogonal polynomials in different interval $(0,1)$ and outside of interval $\mathbb{C}\backslash (0,1)$, respectively; Due to the effect of $\frac{t}{x(1-x)}$ for varying $t$, different asymptotic behaviors at the hard edge $0$ and $1$ were found with different scaling schemes. Specifically, the uniform asymptotic behavior can be expressed as a Airy function in the neighborhood of point $1$ as $\zeta= 2n^2t \to \infty, n\to \infty$, while it is given by a Bessel function as $\zeta \to 0, n \to \infty$. { II. Universality:} We respectively calculate the limit of the eigenvalue correlation kernel in the bulk of the spectrum and at the both side of hard edge, which will involve a $\psi$-functions associated with a particular Painlev$\acute{e}$ \uppercase\expandafter{\romannumeral3} equation near $x=\pm 1$. Further, we also prove the $\psi$-funcation can be approximated by a Bessel kernel as $\zeta \to 0$ compared with a Airy kernel as $\zeta \to \infty$. Our analysis is based on the Deift-Zhou nonlinear steepest descent method for the Riemann-Hilbert problems.
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奇摄动Pollaczek-Jacobi型酉系综的临界边行为
本文研究了奇异摄动Pollaczek-Jacobi型权值$$w_{p_J2}(x,t)=e^{-\frac{t}{x(1-x)}}x^\alpha(1-x)^\beta, $$的正交多项式的强渐近性和普适性,其中$t \ge 0$, $\alpha >0$, $\beta >0$和$x \in [0,1].$,得到的主要结果包括两个方面:{1 .强渐近性:}分别在不同区间$(0,1)$和区间$\mathbb{C}\backslash (0,1)$外得到了一元Pollaczek-Jacobi型正交多项式的强渐近展开式;由于$\frac{t}{x(1-x)}$对$t$的影响,不同标度方案在硬边$0$和$1$处的渐近行为不同。具体地说,一致渐近行为可以表示为在$1$点附近的Airy函数为$\zeta= 2n^2t \to \infty, n\to \infty$,而由Bessel函数为$\zeta \to 0, n \to \infty$给出。{2通用性:}我们分别计算了特征值相关核在光谱主体和硬边两侧的极限,这将涉及与$x=\pm 1$附近的特定Painlev $\acute{e}$\uppercase\expandafter{\romannumeral3}方程相关的$\psi$ -函数。此外,我们还证明了$\psi$ -函数可以用贝塞尔核近似为$\zeta \to 0$,而用艾里核近似为$\zeta \to \infty$。我们的分析是基于Deift-Zhou非线性最陡下降法的黎曼-希尔伯特问题。
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