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

Journal of the Physical Society of Japan

Low-temperature Dephasing and Renormalization in Model Systems (Proceedings of the International Conference on Quantum Transport and Quantum Coherence(Localisation 2002))

Dmitry S. Golubev, Gerd Schön, Andrei D. Zaikin

Published Jan 1, 2003• 0 citations
OpenAlex

Related papers

Electron Decoherence by a Single Spin (Proceedings of the International Conference on Quantum Transport and Quantum Coherence(Localisation 2002))

Pritiraj Mohanty

Journal of the Physical Society of Japan•Jan 1, 2003•0 citations

Decoherence of interacting electrons in disordered conductors: on the relation between influence functional and diagrammatic approaches (Proceedings of the International Conference on Quantum Transport and Quantum Coherence(Localisation 2002))

Jan von Delft

Journal of the Physical Society of Japan•Jan 1, 2003•1 citation

Quantized adiabatic quantum pumping due to interference (Proceedings of the International Conference on Quantum Transport and Quantum Coherence(Localisation 2002))

Ora Entin-wohlman A, Amnon Aharony A, Vyacheslavs Kashcheyevs

Journal of the Physical Society of Japan•Jan 1, 2003•0 citations

Dephasing and Renormalization in Quantum Two-Level Systems

Alexander Shnirman, Gerd Schön

arXiv:cond-mat/0210023•Springer eBooks•Jan 1, 2003•7 citations

Non-universality of dephasing in quantum transport

J. Allinger, U. Weiss

The European Physical Journal B•Jun 1, 1995•7 citations

Localisation determines the optimal noise rate for quantum transport

Alexandre R. Coates, Brendon W. Lovett, Erik M. Gauger

Abstract Environmental noise plays a key role in determining the efficiency of transport in quantum systems. However, disorder and localisation alter the impact of such noise on energy transport. To provide a deeper understanding of this relationship we perform a systematic study of the connection between eigenstate localisation and the optimal dephasing rate in 1D chains. The effects of energy gradients and disorder on chains of various lengths are evaluated and we demonstrate how optimal transport efficiency is determined by both size-independent, as well as size-dependent factors. By discussing how size-dependent influences emerge from finite size effects we establish when these effects are suppressed, and show that a simple power law captures the interplay between size-dependent and size-independent responses. Moving beyond phenomenological pure dephasing, we implement a finite temperature Bloch–Redfield model that captures detailed balance. We show that the relationship between localisation and optimal environmental coupling strength continues to apply at intermediate and high temperature but breaks down in the low temperature limit.

arXiv:2106.12567•New Journal of Physics•Nov 18, 2021•6 citations
Abstract Environmental noise plays a key role in determining the efficiency of transport in quantum systems. However, disorder and localisation alter the impact of such noise on energy transport. To provide a deeper understanding of this relationship we perform a systematic study of the connection between eigenstate localisation and the optimal dephasing rate in 1D chains. The effects of energy gradients and disorder on chains of various lengths are evaluated and we demonstrate how optimal transport efficiency is determined by both size-independent, as well as size-dependent factors. By discussing how size-dependent influences emerge from finite size effects we establish when these effects are suppressed, and show that a simple power law captures the interplay between size-dependent and size-independent responses. Moving beyond phenomenological pure dephasing, we implement a finite temperature Bloch–Redfield model that captures detailed balance. We show that the relationship between localisation and optimal environmental coupling strength continues to apply at intermediate and high temperature but breaks down in the low temperature limit.