The Quantum Symmetric Simple Exclusion Process in the Continuum and Free Processes
Denis Bernard
TL;DR
This work formulates QSSEP directly in the continuum by building a conditioned free-probability framework with diagonal function algebra $L_ty[0,1]$ and free increments, leading to a continuum quantum fluctuating-hydrodynamics description. It develops conditioned free probability, free stochastic calculus, and adjoint-orbit flows to derive unitary evolutions and Lindblad-type mean dynamics, then defines QSSEP in the continuum as the $ 0 o0$ limit of a regularized process with boundary variants (periodic, closed, open). A key result is the equivalence between the continuum QSSEP moments and the large-$N$ scaling limit of the discrete QSSEP, established via closed hierarchies for $oxed{C^{t}_{p+1}}$ and local moments, including explicit open-boundary dynamics. The framework yields invariant measures and non-equal-time correlations, showing conserved global moments in equilibrium-like cases and boundary-driven steady states in open QSSEP, thereby providing a quantum extension of fluctuating hydrodynamics with potential for a quantum mesoscopic fluctuation theory.
Abstract
The quantum symmetric simple exclusion process (QSSEP) is a recent extension of the symmetric simple exclusion process, designed to model quantum coherent fluctuating effects in noisy diffusive systems. It models stochastic nearest-neighbor fermionic hopping on a lattice, possibly driven out-of-equilibrium by boundary processes. We present a direct formulation in the continuum, and establish how this formulation captures the scaling limit of the discrete version. In the continuum, QSSEP emerges as a non-commutative process, driven by free increments, conditioned on the algebra of functions on the ambiant space to encode spatial correlations. We actually develop a more general framework dealing with conditioned orbits with free increments which may find applications beyond the present context. We view this construction as a preliminary step toward formulating a quantum extension of the macroscopic fluctuation theory.
