# Dissipative quantum backflow

## TL;DR

This paper investigates dissipative quantum backflow in open quantum systems using two frameworks, showing that dissipation reduces but does not eliminate backflow, which persists over long times and exhibits unique properties under different conditions.

## Contribution

It provides a comprehensive theoretical analysis of quantum backflow with dissipation, comparing effective Hamiltonian and master equation approaches, and explores its persistence and eigenvalue structure.

## Key findings

- Backflow is reduced by dissipation and temperature but never fully suppressed.
- Quantum backflow persists at long times in the Caldeira-Leggett framework.
- Eigenvalues related to backflow depend on system parameters in the presence of a constant force.

## Abstract

Dissipative backflow is studied in the context of open quantum systems. This theoretical analysis is carried out within two frameworks, the effective time-dependent Hamiltonian due to Caldirola-Kanai (CK) and the Caldeira-Leggett (CL) one where a master equation is used to describe the reduced density matrix in presence of dissipation and temperature of the environment. Two examples are considered, the free evolution of one and two Gaussian wave packets as well as the time evolution under a constant field. Backflow is shown to be reduced with dissipation and temperature but never suppressed. Interestingly enough, quantum backflow is observed when considering both one and two Gaussian wave packets within the CL context. Surprisingly, in both cases, the backflow effect seems to be persistent at long times. Furthermore, the constant force $ m g\geq 0 $ behaves against backflow. However, the classical limit of this quantum effect within the context of the classical Schr\"odinger equation is shown to be present. Backflow is also analyzed as an eigenvalue problem in the Caldirola-Kanai framework. In the free propagation case, eigenvalues are independent on mass, Planck constant, friction and its duration but, in the constant force case, eigenvalues depend on a factor which itself is a combination of all of them as well as the force constant.