Non-intersecting Brownian bridges in the flat-to-flat geometry

TL;DR

This paper analyzes non-intersecting Brownian bridges in a flat-to-flat configuration, deriving exact equations and solutions for their density evolution, and explores connections to integrable models and orthogonal polynomials.

Contribution

It maps the problem to Dyson's Brownian bridges, derives an effective Langevin equation, and solves Burgers' equation for the density evolution in the large N limit.

Findings

Explicit density profiles at specific intermediate times

Effective Langevin equation for efficient sampling

Evolution of density edges from start to end

Abstract

We study $N$ vicious Brownian bridges propagating from an initial configuration $\{a_1 < a_2 < \ldots< a_N \}$ at time $t=0$ to a final configuration $\{b_1 < b_2 < \ldots< b_N \}$ at time $t=t_f$, while staying non-intersecting for all $0\leq t \leq t_f$. We first show that this problem can be mapped to a non-intersecting Dyson's Brownian bridges with Dyson index $\beta=2$. For the latter we derive an exact effective Langevin equation that allows to generate very efficiently the vicious bridge configurations. In particular, for the flat-to-flat configuration in the large $N$ limit, where $a_i = b_i = (i-1)/N$, for $i = 1, \cdots, N$, we use this effective Langevin equation to derive an exact Burgers' equation (in the inviscid limit) for the Green's function and solve this Burgers' equation for arbitrary time $0 \leq t\leq t_f$. At certain specific values of intermediate times $t$, such as $t=t_f/2$, $t=t_f/3$ and $t=t_f/4$ we obtain the average density of the flat-to-flat bridge explicitly. We also derive explicitly how the two edges of the average density evolve from time $t=0$ to time $t=t_f$. Finally, we discuss connections to some well known problems, such as the Chern-Simons model, the related Stieltjes-Wigert orthogonal polynomials and the Borodin-Muttalib ensemble of determinantal point processes.