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

Bulletin of the American Physical Society

Nonequilibrium Kondo physics in the Anderson impurity model: Auxiliary master equation approach

Antonius Dorda, Martin Ganahl, Hans Gerd Evertz, Wolfgang von der Linden, Enrico Arrigoni

Published Mar 16, 2016• 0 citations
OpenAlex

Related papers

Auxiliary master equation approach applied to the nonequilibrium single impurity Anderson model

Antonius Dorda

•Jan 1, 2015•0 citations

Auxiliary master equation approach to the pseudogap Anderson model out of equilibrium

Delia Maria Fugger, Daniel Bauernfeind, Max Erich Sorantin +1 more

•Sep 10, 2019•0 citations

Auxiliary master equation approach for correlated quantum impurities out of equilibrium

Enrico Arrigoni

•Feb 23, 2015•0 citations

Auxiliary master equation approach for correlated quantum impurities out of equilibrium

Irakli Titvinidze, Antonius Dorda, Wolfgang von der Linden +1 more

•Sep 5, 2016•0 citations

Auxiliary master equation approach within matrix product states: Spectral properties of the nonequilibrium Anderson impurity model

Antonius Dorda, Martin Ganahl, Hans Gerd Evertz +2 more

Within the recently introduced auxiliary master equation approach it is possible to address steady state properties of strongly correlated impurity models, small molecules or clusters efficiently and with high accuracy. It is particularly suited for dynamical mean field theory in the nonequilibrium as well as in the equilibrium case. The method is based on the solution of an auxiliary open quantum system, which can be made quickly equivalent to the original impurity problem. In its first implementation a Krylov space method was employed. Here, we aim at extending the capabilities of the approach by adopting matrix product states for the solution of the corresponding auxiliary quantum master equation. This allows for a drastic increase in accuracy and permits us to access the Kondo regime for large values of the interaction. In particular, we investigate the nonequilibrium steady state of a single impurity Anderson model and focus on the spectral properties for temperatures T below the Kondo temperature T_K and for small bias voltages phi. For the two cases considered, with T=T_K/4 and T=T_K/10 we find a clear splitting of the Kondo resonance into a two-peak structure for phi close above T_K. In the equilibrium case (phi=0) and for T=T_K/4, the obtained spectral function essentially coincides with the one from numerical renormalization group.

arXiv:1507.02982•Physical Review B•Sep 24, 2015•79 citations

Kondo correlations formation and the local magnetic moment dynamics in the Anderson model

N. S. Maslova, P. I. Arseyev, Vladimir N. Mantsevich

arXiv:1612.00791•Solid State Communications•Jan 23, 2017•6 citations
Within the recently introduced auxiliary master equation approach it is possible to address steady state properties of strongly correlated impurity models, small molecules or clusters efficiently and with high accuracy. It is particularly suited for dynamical mean field theory in the nonequilibrium as well as in the equilibrium case. The method is based on the solution of an auxiliary open quantum system, which can be made quickly equivalent to the original impurity problem. In its first implementation a Krylov space method was employed. Here, we aim at extending the capabilities of the approach by adopting matrix product states for the solution of the corresponding auxiliary quantum master equation. This allows for a drastic increase in accuracy and permits us to access the Kondo regime for large values of the interaction. In particular, we investigate the nonequilibrium steady state of a single impurity Anderson model and focus on the spectral properties for temperatures T below the Kondo temperature T_K and for small bias voltages phi. For the two cases considered, with T=T_K/4 and T=T_K/10 we find a clear splitting of the Kondo resonance into a two-peak structure for phi close above T_K. In the equilibrium case (phi=0) and for T=T_K/4, the obtained spectral function essentially coincides with the one from numerical renormalization group.