Reunion probabilities of $N$ one-dimensional random walkers with mixed boundary conditions

TL;DR

This paper extends the analysis of reunion probabilities for N one-dimensional random walkers to include mixed boundary conditions, using Quantum Mechanics formalism and Bethe ansatz to derive new expressions applicable to various boundary scenarios.

Contribution

It introduces a unified framework for calculating reunion probabilities of random walkers with mixed boundary conditions using quantum formalism and Bethe ansatz techniques.

Findings

Derived explicit formulas for reunion probabilities with mixed boundary conditions.

Connected the problem to Lieb-Liniger gas and Bethe equations.

Extended known results to new boundary condition models.

Abstract

In this work we extend the results of the reunion probability of $N$ one-dimensional random walkers to include mixed boundary conditions between their trajectories. The level of the mixture is controlled by a parameter $c$, which can be varied from $c=0$ (independent walkers) to $c\to\infty$ (vicious walkers). The expressions are derived by using Quantum Mechanics formalism (QMf) which allows us to map this problem into a Lieb-Liniger gas (LLg) of $N$ one-dimensional particles. We use Bethe ansatz and Gaudin's conjecture to obtain the normalized wave-functions and use this information to construct the propagator. As it is well-known, depending on the boundary conditions imposed at the endpoints of a line segment, the statistics of the maximum heights of the reunited trajectories have some connections with different ensembles in Random Matrix Theory (RMT). Here we seek to extend those results and consider four models: absorbing, periodic, reflecting, and mixed. In all four cases, the probability that the maximum height is less or equal than $L$ takes the form $F_N(L)=A_N\sum_{k\in\Omega_{B}}\int Dz e^{-\sum_{j=1}^Nk_j^2+G_N(k)-\sum_{j,\ell=1}^N z_jV_{j\ell}(k)\overline{z}_\ell}$, where $A_N$ is a normalization constant, $G_N(k)$ and $V_{j\ell}(k)$ depend on the type of boundary condition, and $\Omega_{B}$ is the solution set of quasi-momenta $k$ obeying the Bethe equations for that particular boundary condition.