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

arXiv:1602.04045 · Communications in Mathematical Physics

Scattering Theory for Lindblad Master Equations

Marco Falconi, Jérémy Faupin, Jürg Martin Fröhlich, Baptiste Schubnel

Published Aug 30, 2016• 18 citations
arXivHTMLPDF
DOI
10.1007/s00220-016-2737-1

Related papers

A solution ansatz for Lindblad master equation with a dynamical system theory approach

Gehad Sadiek, E. I. Lashin

Bulletin of the American Physical Society•Mar 4, 2019•0 citations

Exploring the theory of open quantum systems: The Lindblad master equation and Decoherence

Giovanni van Marion

•Jul 6, 2018•0 citations

Validity of the Lindblad master equations

Tuure Orell

•Jan 1, 2017•0 citations

The Matrix Perturbation Method for the Lindblad Master Equation

Francisco Soto, Braulio Misael Villegas-Martínez, H. M. Moya-Cessa

Springer eBooks•Jan 1, 2023•0 citations

Lindblad Plus From Feynman-Vernon

Jose A. Magpantay

I show how the Lindblad Plus equation will follow from the Feynman-Vernon theory. The Plus refers to the inclusion of non-Markov processes in the Lindblad equation resulting in an integro-differential general master equation. The equivalence of this general master equation and not the Lindblad equation alone to the Feynman-Vernon theory should be expected because the sum over histories approach of the FV theory clearly includes non-Markov processes, which Lindblad equation ignores. This should close the seeming gap between these two approaches to quantum open systems.

arXiv:2003.00194•Feb 29, 2020•0 citations

Quantum Trajectories for Time-Local Non-Lindblad Master Equations

Tobias Becker, Ché Netzer, André Eckardt

For the efficient simulation of open quantum systems, we often use quantum jump trajectories given by pure states that evolve stochastically to unravel the dynamics of the underlying master equation. In the Markovian regime, when the dynamics is described by a Gorini-Kossakowski-Sudarshan-Lindblad (GKSL) master equation, this procedure is known as Monte Carlo wave function approach. However, beyond ultraweak system-bath coupling, the dynamics of the system is not described by an equation of GKSL type, but rather by the Redfield equation, which can be brought into pseudo-Lindblad form. Here, negative dissipation strengths prohibit the conventional approach. To overcome this problem, we propose a pseudo-Lindblad quantum trajectory (PLQT) unraveling. It does not require an effective extension of the state space, like other approaches, except for the addition of a single classical bit. We test the PLQT for the eternal non-Markovian master equation for a single qubit and an interacting Fermi-Hubbard chain coupled to a thermal bath and discuss its computational effort compared to solving the full master equation.

arXiv:2306.14876•Physical Review Letters•Oct 17, 2023•11 citations
I show how the Lindblad Plus equation will follow from the Feynman-Vernon theory. The Plus refers to the inclusion of non-Markov processes in the Lindblad equation resulting in an integro-differential general master equation. The equivalence of this general master equation and not the Lindblad equation alone to the Feynman-Vernon theory should be expected because the sum over histories approach of the FV theory clearly includes non-Markov processes, which Lindblad equation ignores. This should close the seeming gap between these two approaches to quantum open systems.
For the efficient simulation of open quantum systems, we often use quantum jump trajectories given by pure states that evolve stochastically to unravel the dynamics of the underlying master equation. In the Markovian regime, when the dynamics is described by a Gorini-Kossakowski-Sudarshan-Lindblad (GKSL) master equation, this procedure is known as Monte Carlo wave function approach. However, beyond ultraweak system-bath coupling, the dynamics of the system is not described by an equation of GKSL type, but rather by the Redfield equation, which can be brought into pseudo-Lindblad form. Here, negative dissipation strengths prohibit the conventional approach. To overcome this problem, we propose a pseudo-Lindblad quantum trajectory (PLQT) unraveling. It does not require an effective extension of the state space, like other approaches, except for the addition of a single classical bit. We test the PLQT for the eternal non-Markovian master equation for a single qubit and an interacting Fermi-Hubbard chain coupled to a thermal bath and discuss its computational effort compared to solving the full master equation.