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  • Open Access

Coherent Fluctuations in Noisy Mesoscopic Systems, the Open Quantum SSEP, and Free Probability

Ludwig Hruza and Denis Bernard
Phys. Rev. X 13, 011045 – Published 24 March 2023

Abstract

Quantum coherences characterize the ability of particles to quantum mechanically interfere within some given distances. In the context of noisy many-body quantum systems, these coherences can fluctuate. A simple toy model to study such fluctuations in an out-of-equilibrium setting is the open quantum symmetric simple exclusion process (Q-SSEP), which describes spinless fermions in one dimension hopping to neighboring sites with random amplitudes coupled between two reservoirs. Here, we show that the dynamics of fluctuations of coherences in Q-SSEP have a natural interpretation as free cumulants, a concept from free probability theory. Based on this insight, we provide heuristic arguments as to why we expect free probability theory to be an appropriate framework to describe coherent fluctuations in generic mesoscopic systems where the noise emerges from a coarse-grained description. In the case of Q-SSEP, we show how the link to free probability theory can be used to derive the time evolution of connected fluctuations of coherences as well as a simple steady-state solution.

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  • Received 5 May 2022
  • Revised 5 December 2022
  • Accepted 17 January 2023

DOI:https://doi.org/10.1103/PhysRevX.13.011045

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Statistical Physics & Thermodynamics

Authors & Affiliations

Ludwig Hruza* and Denis Bernard

  • Laboratoire de Physique de l’École Normale Supérieure, CNRS, ENS & PSL University, Sorbonne Université, Université Paris Cité, 75005 Paris, France

  • *ludwig.hruza@ens.fr
  • denis.bernard@ens.fr

Popular Summary

The characterization of nonequilibrium systems from the point of view of statistical mechanics is an enduring challenge in theoretical physics. Since such systems usually depend on a variety of system-specific details, there are no general formulas for the probability of microscopic configurations. Usually, one is interested in the statistics of measurable, macroscopic quantities such as the particle density or current. However, if the size of such systems is very small, quantum mechanical effects can become important, and they can affect macroscopic quantities. Here, we show that the fluctuations of these quantum mechanical effects have a universal description that applies to generic mesoscopic and diffusive systems.

We study a toy mathematical model that provides the minimal structure necessary to describe the fluctuations of quantum mechanical effects in diffusive, nonequilibrium, many-body quantum systems. We show that these fluctuations have a natural mathematical description in terms of tools from free probability theory, a framework that deals with noncommuting random variables—a feature also central to quantum mechanics. Furthermore, we argue why we expect this connection to hold for generic mesoscopic systems, and we interpret the emergence of free probability theory in our toy model as a sign that the model could indeed encode universal fluctuations of a larger class of systems.

Free probability has also been observed in the context of the eigenstate thermalization hypothesis—a set of ideas to explain why an isolated quantum mechanical system can be described using equilibrium statistical mechanics—and we expect that its tools will play an important role in the understanding of chaotic or noisy many-body quantum systems.

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Vol. 13, Iss. 1 — January - March 2023

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  • Figure 1
    Figure 1

    Schematic representation of a mesoscopic system coupled to two reservoirs of different chemical potentials μa and μb. Here, denotes the ballistic length, above which the transport is diffusive, and Lϕ is the coherence length, below which interference effects can be observed.

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  • Figure 2
    Figure 2

    Cells around sites i and j in the mesoscopic system corresponding to single sites in the coarse-grained description. The toy model Q-SSEP seems to be a good candidate for such a coarse-grained description. Noise emerges by averaging the mesoscopic system over all unitary transformations that only act on the individual cells, and it conserves the number of particles inside each cell.

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  • Figure 3
    Figure 3

    Discrete fermion density nLx(L2t) for system sizes L=24 and L=48, together with the scaling limit ρ(x,t) at t=0.01 as a function of space x=i/L. The extraction and injection rates are α1=β1=αL=βL=1, and they do not fit the initial conditions. The agreement is very good.

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  • Figure 4
    Figure 4

    Boundary conditions that fit the initial domain wall state (na=1, nb=0).

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  • Figure 5
    Figure 5

    Boundary conditions that do not fit the initial domain wall state (na=1/2, nb=1/2).

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  • Figure 6
    Figure 6

    Two wires attached to the system at sites i and j such that only one fermion can enter at a time. First, the fermions in the wire are allowed to interact via the beam splitter S. Then, their occupation numbers nL and nR are measured on each side. In the first measurement (a), one uses a symmetric beam splitter, which allows one to measure the imaginary part of Gij. In the second measurement (b), one needs to use a beam splitter where the fermion that is transmitted from R to L accumulates a phase π, while it does not accumulate this phase when being transmitted in the other direction. In this way, one can measure the real part of Gij.

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