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Some freezing limits for Bessel functions and Bessel processes with drift of type BNB_N

Jan Richter, Michael Voit

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Source: arXiv

Published: Sep 17, 2026

arXiv: 2609.21071

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Source abstract

We use the series representation of the Bessel functions of type BNB_N in terms of Jack polynomials and show that limk1J(k1,k2)B(x,k1y)1/k1=2Ni=1N(e1+xi2yi2111+xi2yi2+1)\lim_{k_1\to\infty} J_{(k_1,k_2)}^B(x,k_1y)^{1/k_1}= 2^N\prod\limits_{i=1}^N \Bigg( e^{\sqrt{1+x_i^2 y_i^2}-1}\cdot \frac{1}{\sqrt{1+x_i^2 y_i^2}+1} \Bigg) for x,yRNx,y\in\mathbb R^N and k20k_2\ge0. Moreover, the known Laplace-type integral representations for N1N\ge1 and k2=0,1/2,1,2k_2=0,1/2,1,2 and for N=2N=2 and k2>0k_2>0 by Rösler and Demni respectively lead to related limits for limk1xjJ(k1,k2)B(x,k1y)/(k1J(k1,k2)B(x,k1y))(j=1,,N).\lim_{k_1 \to \infty} \partial_{x_j} J_{(k_1,k_2)}^B(x,k_1y) /(k_1 \cdot J_{(k_1,k_2)}^B(x,k_1 y)) \quad (j=1,\ldots,N). These limits lead to weak limit results for the associated Bessel processes with drift. For k2=1/2,1,2k_2=1/2,1,2, these limit results have applications to radial parts of Brownian motions with drift on the M×NM\times N-dimensional matrices over R,C\mathbb R,\mathbb C, and the quaternions for MM\to\infty. We also discuss these limits in the Dunkl case N=1N=1.

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