Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Springer eBooks

Heisenberg equation-of-motion methods applied to non-Markovian open systems

James D. Cresser

Published Jan 1, 2003• 2 citations
Publisher
DOI
10.1007/978-1-4419-8907-9_159

Related papers

Non-Markovian dynamics of open quantum systems

Carole Addis

•Oct 1, 2016•7 citations

A Heisenberg equation-of-motion derivation of stochastic Schrödinger equations for non-markovian open systems

James D. Cresser

A method is presented by which the stochastic Schrodinger equation can be derived for systems coupled to a reservoir in cases in which the system-reservoir interaction is non-Markovian, and under the condition that the initial system reservoir state is decorrelated. The method is based on a Heisenberg equation of motion approach applied in conjunction with a technique of dealing with system-reservoir interactions introduced by Mollow in his treatment of the AC Stark effect. The general Diosi-Strunz stochastic Schrodinger equation is regained, but the method developed here offers a different perspective on obtaining the final form of this equation for specific applications. The method is illustrated for a damped two level atom, a driven damped harmonic oscillator, and quantum Brownian motion.

Laser Physics•Jan 1, 2000•13 citations

Investigating non-Markovian dynamics of quantum open systems

Yusui Chen

•Jan 1, 2015•0 citations

Time-evolution operator method for non-Markovian density matrix propagation in time and space representation: Application to laser association of OH in an environment

G. K. Paramonov, Peter Saalfrank

An efficient method for the numerical solution of a non-Markovian, open-system density matrix equation of motion in coordinate representation is developed. We apply the scheme to model simulations of the laser-assisted $\mathrm{O}+\mathrm{H}\ensuremath{\rightarrow}\mathrm{O}\mathrm{H}$ association reaction in an environment. The suggested approach is based on the application of the time-evolution operator to the ``closed-system'' part of the overall Hamiltonian and transformation of the open-system equation of motion to the Heisenberg picture suitable for numerical propagation. A dual role of the system-environment coupling with respect to the infrared (ir) laser-driven association of OH is demonstrated: the association probability is increased due to the coupling at relatively weak laser fields, but decreased at strong laser fields. Moreover, at a certain strength of the ir laser field, the association probability does not depend on the strength of the system-bath coupling at all.

Physical Review A•Jan 16, 2009•10 citations

Dynamics of non-Markovian open quantum systems

Inés de Vega, Daniel Alonso

This review gives a summary of the many techniques that are used in the analysis of open quantum systems. Emphasis is on those cases where it is unsuitable to use a memoryless or Markovian point of view, generally because there is no large separation of time scales between system and environment dynamics. The approaches reviewed include master equations, Heisenberg equations of motion, chain mapping representations, and various stochastic methods such as path integral Monte Carlo and stochastic equations. Guidance is given on how to evaluate the suitability of each of these methods for application in different physical problems.

arXiv:1511.06994•Reviews of Modern Physics•Jan 20, 2017•1,230 citations

The non-Markovian stochastic Schrödinger equation for open systems

Lajos Diósi, Walter T. Strunz

arXiv:quant-ph/9706050•Physics Letters A•Nov 1, 1997•283 citations
A method is presented by which the stochastic Schrodinger equation can be derived for systems coupled to a reservoir in cases in which the system-reservoir interaction is non-Markovian, and under the condition that the initial system reservoir state is decorrelated. The method is based on a Heisenberg equation of motion approach applied in conjunction with a technique of dealing with system-reservoir interactions introduced by Mollow in his treatment of the AC Stark effect. The general Diosi-Strunz stochastic Schrodinger equation is regained, but the method developed here offers a different perspective on obtaining the final form of this equation for specific applications. The method is illustrated for a damped two level atom, a driven damped harmonic oscillator, and quantum Brownian motion.
An efficient method for the numerical solution of a non-Markovian, open-system density matrix equation of motion in coordinate representation is developed. We apply the scheme to model simulations of the laser-assisted $\mathrm{O}+\mathrm{H}\ensuremath{\rightarrow}\mathrm{O}\mathrm{H}$ association reaction in an environment. The suggested approach is based on the application of the time-evolution operator to the ``closed-system'' part of the overall Hamiltonian and transformation of the open-system equation of motion to the Heisenberg picture suitable for numerical propagation. A dual role of the system-environment coupling with respect to the infrared (ir) laser-driven association of OH is demonstrated: the association probability is increased due to the coupling at relatively weak laser fields, but decreased at strong laser fields. Moreover, at a certain strength of the ir laser field, the association probability does not depend on the strength of the system-bath coupling at all.
This review gives a summary of the many techniques that are used in the analysis of open quantum systems. Emphasis is on those cases where it is unsuitable to use a memoryless or Markovian point of view, generally because there is no large separation of time scales between system and environment dynamics. The approaches reviewed include master equations, Heisenberg equations of motion, chain mapping representations, and various stochastic methods such as path integral Monte Carlo and stochastic equations. Guidance is given on how to evaluate the suitability of each of these methods for application in different physical problems.