Linear statistics at the microscopic scale for the 2D Coulomb gas
arXiv:2503.18586 · doi:10.1088/1751-8121/ae11e2
Abstract
We consider the classical Coulomb gas in two dimensions at the inverse temperature , confined within a droplet of radius by a rotationally invariant potential . For this describes the eigenvalues of the complex Ginibre ensemble of random matrices. We study linear statistics of the form , where 's are the positions of the particles, in the large limit with . It is known that for smooth functions the variance , while for an indicator function relevant for the disk counting statistics, all cumulants of of order behave as . In addition, for smooth functions, it was shown that the cumulants of of order scale as . Surprisingly it was found that they depend only on and its derivatives evaluated exactly at the boundary of the droplet. To understand this property, and interpolate between the two behaviors (smooth versus step-like), we study the microscopic linear statistics given by , which probes the fluctuations at the scale of the inter-particle distance. We compute the cumulants of at large for a fixed at arbitrary . For large they match the predictions for smooth functions which shows that the leading contribution in that case comes from a boundary layer of size near the boundary of the droplet. Finally we show that the full probability distribution of take two distinct large deviation forms, in the regime and respectively. We also discuss applications of our results to fermions in a rotating harmonic trap and to the Ginibre symplectic ensemble.
40 pages, 7 figures
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