Information Loss Pathways in a Numerically Exact Simulation of a non-Markovian Open Quantum System

TL;DR

This paper develops a numerical method to simulate non-Markovian open quantum systems without revivals by introducing the concept of memory channels, which account for irreversible information loss at spectral singularities.

Contribution

It introduces a novel discretization approach that separates observable and virtual quanta, employing stochastic sampling and delay-time representations to eliminate simulation revivals.

Findings

Successfully avoids revivals in simulations of non-Markovian dynamics.

Identifies the role of spectral singularities in information loss.

Provides a new framework for representing virtual quantum states.

Abstract

In the non-Markovian regime, the bath has the memory about the past behavior of the open quantum system. This memory has slowly-decaying power-law tails. Such a long-range character of the memory complicates the description of the resulting real-time dynamics on large time scales. In a numerical simulation, this problem manifests itself in a `revival', a spurious reflected signal which appears after a finite time thus invalidating the simulation. In the present work, we approach this problem and develop a numerical discretization of the bath without revivals. We find that a crucial role is played by the singularities of the bath spectral density (e.g. edges of bands): the memory about the (spectral) behaviour of the open system in the remote past is completely averaged out (forgotten), except an increasingly small vicinity of these singular frequencies. Therefore, we introduce the concept of memory channel, to denote such an irreversible information loss process around a particular singular frequency. On a technical side, we begin the treatment by noting that with respect to the memory loss, the quantum field of the bath should be divided into the following two different parts: the observable and the virtual quanta. Information about the former is never lost: they contribute to the trace over the bath degrees of freedom. The only way to avoid the revival from the observable quanta is to calculate their dynamics exactly. We do this by employing a stochastic sampling of the Husimi function of the bath. The other part, the virtual quanta, are always annihilated after a certain delay time. We construct a dedicated quantum representation for the virtual states by assigning amplitudes to the delay times before annihilation. It is in this representation we rigorously define the concept of memory channels.