Abstract

In [16], a solvable two charge ensemble of interacting charged particles on the real line in the presence of the harmonic oscillator potential is introduced. It can be seen as a special form of a grand canonical ensemble with the total charge being fixed and unit charge particles being random. Moreover, it serves as an interpolation between the Gaussian orthogonal and the Gaussian symplectic ensembles and maintains the Pfaffian structure of the eigenvalues. A similar solvable ensemble of charged particles on the unit circle was studied in [17, 10]. In this paper we explore the sharp asymptotic behavior of the number of unit charge particles on the line and on the circle, as the total charge goes to infinity. We establish extended central limit theorems, Berry-Esseen estimates and precise moderate deviations using the machinery of the mod-Gaussian convergence developed in [6, 15, 14, 4, 7]. Also a large deviation principle is derived using the Gärtner-Ellis theorem.

Highlights

  • We first present a general model of charged particles with charge ratio 1 : 2 interacting via a logarithmic potential

  • We study the distribution of the number of charge one particles for the proper scaling of the parameter X, when the total charge N tends to infinity

  • The case X = 1 has been studied in details in [16] and the limiting results such as CLT and large deviation principle (LDP) have been derived. We extend their results by proving mod-Gaussian convergence for the sequence and deducing all its consequences such as precise moderate deviations and extended central limit theorem

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Summary

Introduction

We first present a general model of charged particles with charge ratio 1 : 2 interacting via a logarithmic potential. Let L, M, N be non-negative integers such that L + 2M = N. The two-component log-gas to be considered consists of L particles with unit charge and M particles with charge two, located either on the line or on the unit circle and interacting via the logarithmic potential. 1≤i

The total energy is then
We conclude that
With tn
The first derivative is clearly
We set n
Kowalski and
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