Parametric representation of open quantum systems and crossover from quantum to classical environment

TL;DR

This paper introduces a parametric method using generalized coherent states to study open quantum systems, enabling the tracking of the quantum-to-classical transition of the environment and its effects on a central qubit.

Contribution

It presents a novel approach to model open quantum systems that captures the crossover from quantum to classical environments through environmental coherent states.

Findings

The qubit behaves as if under an external magnetic field influenced by environmental states.

The environmental quantum character narrows with increasing total spin S, approaching a classical limit.

Entanglement remains well-defined even as the environment becomes classical, related to the Berry phase.

Abstract

We propose an approach to the study of open quantum systems based on a parametric representation of the principal system. The representation is obtained introducing generalized coherent states for the environment, and is such that the evolution from a fully quantum environment to a classical one can be inherently followed. The method is applied to the specific case where the principal system is a central qubit and the environment is a surrounding ring of interacting spins, with the overall Hamiltonian being that of the $s=1/2$ Heisenberg star with frustration. In this case the quantum character of the environment, embodied by the total spin $S$ of the ring, can be physically varied by acting on the ratio between the couplings entering the Hamiltonian, and formally followed by increasing $S$. We find that when the star is in any of its eigenstates, the qubit behaves as if it were under the effect of an external magnetic field, whose direction in real space is set by the variables defining the environmental coherent states, and is hence broadened according to their quantum probability distribution. When the quantum character of the environment is reduced, such distribution becomes narrower, finally collapsing into a Dirac-$\delta$ as $S\to\infty$. The entanglement between the central qubit and its environment remains well defined even in this limit, where it comes across as the binary entropy of the $2\pi$-normalized Berry phase characterizing the dynamics of a qubit in an adiabatically precessing magnetic field.