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Exact solution of an integrable non-equilibrium particle system

Rouven Frassek, Cristian Giardinà

Abstract

We consider the integrable family of symmetric boundary-driven interacting particle systems that arise from the non-compact XXX Heisenberg model in one dimension with open boundaries. In contrast to the well-known symmetric exclusion process, the number of particles at each site is unbounded. We show that a finite chain of $N$ sites connected at its ends to two reservoirs can be solved exactly, i.e. the factorial moments of the non-equilibrium steady-state can be written in closed form for each $N$. The solution relies on probabilistic arguments and techniques inspired by integrable systems. It is obtained in two steps: i) the introduction of a dual absorbing process reducing the problem to a finite number of particles; ii) the solution of the dual dynamics exploiting a symmetry obtained from the Quantum Inverse Scattering Method. Long-range correlations are computed in the finite-volume system. The exact solution allows to prove by a direct computation that, in the thermodynamic limit, the system approaches local equilibrium. A by-product of the solution is the algebraic construction of a direct mapping between the non-equilibrium steady state and the equilibrium reversible measure.

Exact solution of an integrable non-equilibrium particle system

Abstract

We consider the integrable family of symmetric boundary-driven interacting particle systems that arise from the non-compact XXX Heisenberg model in one dimension with open boundaries. In contrast to the well-known symmetric exclusion process, the number of particles at each site is unbounded. We show that a finite chain of sites connected at its ends to two reservoirs can be solved exactly, i.e. the factorial moments of the non-equilibrium steady-state can be written in closed form for each . The solution relies on probabilistic arguments and techniques inspired by integrable systems. It is obtained in two steps: i) the introduction of a dual absorbing process reducing the problem to a finite number of particles; ii) the solution of the dual dynamics exploiting a symmetry obtained from the Quantum Inverse Scattering Method. Long-range correlations are computed in the finite-volume system. The exact solution allows to prove by a direct computation that, in the thermodynamic limit, the system approaches local equilibrium. A by-product of the solution is the algebraic construction of a direct mapping between the non-equilibrium steady state and the equilibrium reversible measure.

Paper Structure

This paper contains 41 sections, 19 theorems, 255 equations, 2 figures.

Key Result

Proposition \oldthetheorem

Denote the reservoir densities by Define the duality function $D: {\mathscr C}_{N}\times {\mathscr C}_{N+2} \to \mathbb{R}$ Then, for any time $t>0$ and for every configurations $m\in{\mathscr C}_{N}$ and $\xi\in{\mathscr C}_{N+2}$, we have the equality

Figures (2)

  • Figure 1: Example of a Young diagram corresponding to the positions $x=(2,2,2,4,7)$ and occupations $m=(0,3,0,1,0,0,1)$.
  • Figure 2: Example of a Young subdiagram corresponding to the positions $\hat{x}=(2,2,7)$ and occupations $\eta=(0,2,0,0,0,0,1)$

Theorems & Definitions (52)

  • Definition \oldthetheorem: The process
  • Remark : Existence of the process
  • Remark : Shifted harmonic numbers
  • Definition \oldthetheorem: Stationary state
  • Definition \oldthetheorem: The dual process
  • Proposition \oldthetheorem: Duality
  • Definition \oldthetheorem: Scaled factorial moments
  • Proposition \oldthetheorem: Scaled factorial moments via absorption probabilities
  • Theorem \oldthetheorem: Scaled factorial moments
  • Remark : Half-integer spin values
  • ...and 42 more