{"title":"随机正态矩阵:硬墙附近的特征值相关性","authors":"Yacin Ameur, Christophe Charlier, Joakim Cronvall","doi":"10.1007/s10955-024-03314-8","DOIUrl":null,"url":null,"abstract":"<p>We study pair correlation functions for planar Coulomb systems in the pushed phase, near a ring-shaped impenetrable wall. We assume coupling constant <span>\\(\\Gamma =2\\)</span> and that the number <i>n</i> of particles is large. We find that the correlation functions decay slowly along the edges of the wall, in a narrow interface stretching a distance of order 1/<i>n</i> from the hard edge. At distances much larger than <span>\\(1/\\sqrt{n}\\)</span>, the effect of the hard wall is negligible and pair correlation functions decay very quickly, and in between sits an interpolating interface that we call the “semi-hard edge”. More precisely, we provide asymptotics for the correlation kernel <span>\\(K_{n}(z,w)\\)</span> as <span>\\(n\\rightarrow \\infty \\)</span> in two microscopic regimes (with either <span>\\(|z-w| = \\mathcal{O}(1/\\sqrt{n})\\)</span> or <span>\\(|z-w| = \\mathcal{O}(1/n)\\)</span>), as well as in three macroscopic regimes (with <span>\\(|z-w| \\asymp 1\\)</span>). For some of these regimes, the asymptotics involve oscillatory theta functions and weighted Szegő kernels.</p>","PeriodicalId":667,"journal":{"name":"Journal of Statistical Physics","volume":null,"pages":null},"PeriodicalIF":1.3000,"publicationDate":"2024-08-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Random Normal Matrices: Eigenvalue Correlations Near a Hard Wall\",\"authors\":\"Yacin Ameur, Christophe Charlier, Joakim Cronvall\",\"doi\":\"10.1007/s10955-024-03314-8\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>We study pair correlation functions for planar Coulomb systems in the pushed phase, near a ring-shaped impenetrable wall. We assume coupling constant <span>\\\\(\\\\Gamma =2\\\\)</span> and that the number <i>n</i> of particles is large. We find that the correlation functions decay slowly along the edges of the wall, in a narrow interface stretching a distance of order 1/<i>n</i> from the hard edge. At distances much larger than <span>\\\\(1/\\\\sqrt{n}\\\\)</span>, the effect of the hard wall is negligible and pair correlation functions decay very quickly, and in between sits an interpolating interface that we call the “semi-hard edge”. More precisely, we provide asymptotics for the correlation kernel <span>\\\\(K_{n}(z,w)\\\\)</span> as <span>\\\\(n\\\\rightarrow \\\\infty \\\\)</span> in two microscopic regimes (with either <span>\\\\(|z-w| = \\\\mathcal{O}(1/\\\\sqrt{n})\\\\)</span> or <span>\\\\(|z-w| = \\\\mathcal{O}(1/n)\\\\)</span>), as well as in three macroscopic regimes (with <span>\\\\(|z-w| \\\\asymp 1\\\\)</span>). For some of these regimes, the asymptotics involve oscillatory theta functions and weighted Szegő kernels.</p>\",\"PeriodicalId\":667,\"journal\":{\"name\":\"Journal of Statistical Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2024-08-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Statistical Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1007/s10955-024-03314-8\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, MATHEMATICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Statistical Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1007/s10955-024-03314-8","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
Random Normal Matrices: Eigenvalue Correlations Near a Hard Wall
We study pair correlation functions for planar Coulomb systems in the pushed phase, near a ring-shaped impenetrable wall. We assume coupling constant \(\Gamma =2\) and that the number n of particles is large. We find that the correlation functions decay slowly along the edges of the wall, in a narrow interface stretching a distance of order 1/n from the hard edge. At distances much larger than \(1/\sqrt{n}\), the effect of the hard wall is negligible and pair correlation functions decay very quickly, and in between sits an interpolating interface that we call the “semi-hard edge”. More precisely, we provide asymptotics for the correlation kernel \(K_{n}(z,w)\) as \(n\rightarrow \infty \) in two microscopic regimes (with either \(|z-w| = \mathcal{O}(1/\sqrt{n})\) or \(|z-w| = \mathcal{O}(1/n)\)), as well as in three macroscopic regimes (with \(|z-w| \asymp 1\)). For some of these regimes, the asymptotics involve oscillatory theta functions and weighted Szegő kernels.
期刊介绍:
The Journal of Statistical Physics publishes original and invited review papers in all areas of statistical physics as well as in related fields concerned with collective phenomena in physical systems.