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A point process on the unit circle with antipodal interactions

Probability 2025-03-03 v3 Mathematical Physics math.MP

Abstract

We introduce the point process \begin{align*} \frac{1}{Z_{n}}\prod_{1 \leq j < k \leq n} |e^{i\theta_{j}}+e^{i\theta_{k}}|^{\beta}\prod_{j=1}^{n} d\theta_{j}, \qquad \theta_{1},\ldots,\theta_{n} \in (-\pi,\pi], \quad \beta > 0, \end{align*} where ZnZ_{n} is the normalization constant. This point process is attractive: it involves nn dependent, uniformly distributed random variables on the unit circle that attract each other. (For comparison, the well-studied Cβ\betaE involves nn uniformly distributed random variables on the unit circle that repel each other.) We consider linear statistics of the form j=1ng(θj)\sum_{j=1}^{n}g(\theta_{j}) as nn \to \infty, where gC1,qg\in C^{1,q} and 2π2\pi-periodic. We prove that the leading order fluctuations around the mean are of order nn and given by (g(U)ππg(θ)dθ2π)n\smash{\big(g(U)-\int_{-\pi}^{\pi}g(\theta) \frac{d\theta}{2\pi}}\big)n, where UUniform(π,π]U \sim \mathrm{Uniform}(-\pi,\pi]. We also prove that the subleading fluctuations around the mean are of order n\sqrt{n} and of the form NR(0,4g(U)2/β)n\mathcal{N}_{\mathbb{R}}(0,4g'(U)^{2}/\beta)\sqrt{n}, i.e. that the subleading fluctuations are given by a Gaussian random variable that itself has a random variance. Our proof uses techniques developed by McKay and Isaev [8,6] to obtain asymptotics of related nn-fold integrals.

Keywords

Cite

@article{arxiv.2212.06787,
  title  = {A point process on the unit circle with antipodal interactions},
  author = {Christophe Charlier},
  journal= {arXiv preprint arXiv:2212.06787},
  year   = {2025}
}

Comments

Results are improved; 12 pages, 1 figure

R2 v1 2026-06-28T07:32:52.540Z