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

Quantum information protocols and thermodynamics with open quantum systems

Sina Hamedani Raja

Published Dec 15, 2020• 0 citations
OpenAlex

Related papers

Thermodynamics of Open Quantum Systems

Juliette Monsel

Springer theses•Jan 1, 2020•0 citations

Thermodynamic description of non-Markovian information flux of nonequilibrium open quantum systems

Hongbin Chen, Guang-Yin Chen, Yueh-Nan Chen

One of the fundamental issues in the field of open quantum systems is the classification and quantification of non-Markovianity. In the contest of quantity-based measures of non-Markovianity, the intuition of non-Markovianity in terms of information backflow is widely discussed. However, it is not easy to characterize the information flux for a given system state and show its connection to non-Markovianity. Here, by using the concepts from thermodynamics and information theory, we discuss a potential definition of information flux of an open quantum system, valid for static environments. We present a simple protocol to show how a system attempts to share information with its environment and how it builds up system-environment correlations. We also show that the information returned from the correlations characterizes the non-Markovianity and a hierarchy of indivisibility of the system dynamics.

arXiv:1707.05521•Physical Review A•Dec 11, 2017•22 citations

Thermodynamic Uncertainty of Work in Time-Dependently Driven Open Quantum Systems

Chulan Kwon

We derive a thermodynamic uncertainty relation for work in an open quantum system driven by a time-dependent protocol and subject to repeated projective energy measurements. The protocol is represented by a sequence of protocol quenches separated by finite-time Lindblad evolution, so that work is accumulated at the quenches while dissipation occurs between them. The resulting work statistics obey the Gallavotti-Cohen symmetry to give rise to the Crooks and Jarzynski fluctuation relations. By perturbing the dissipative dynamics and combining the Cramér--Rao inequality with the quantum Fisher information, we obtain $\mathrm{Var}\,W/[τ\partial_τ\langle W\rangle]^2\ge 1/F\ge\max(1/A,2/E)$, where $\langle W\rangle$ is the work expectation value, $\mathrm{Var}\,W$ is the variance of work, $F$ is the Fisher information, $A$ is the dynamical activity, $E$ is the dimensionless entropy production, and $τ$ is the switching time interval between quenches. The two thermodynamic bounds follow from two independent perturbations that generate the same response of the work statistics. We illustrate the relation for a dissipative two-level system under square-wave and sinusoidal driving and show that the tighter thermodynamic bound can depend on the driving protocol and switching time scale.

quant-pharXiv:2609.17032•Sep 16, 2026•0 citations

Thermodynamics of quantum information

Sebastian Deffner, Steve Campbell

Morgan & Claypool Publishers eBooks•Jul 1, 2019•8 citations

Quantum Information Concepts in Open Quantum Systems

Bassano Vacchini, Andrea Smirne, Nina Megier

This issue contains contributions in different cutting edge topics within the field of open quantum systems. The theoretical work presented is focused, in particular, on quantum thermodynamics and quantum non-Markovianity and provides a window into current research in these fields. Different perspectives are considered that share a common root in the exploitation of open quantum systems and quantum information tools.

MDPI eBooks•Feb 3, 2023•0 citations

Quantum Thermodynamics of Information

Austin K. Daniel, Yuri V. Rostovtsev

Bulletin of the American Physical Society•Apr 2, 2016•0 citations
One of the fundamental issues in the field of open quantum systems is the classification and quantification of non-Markovianity. In the contest of quantity-based measures of non-Markovianity, the intuition of non-Markovianity in terms of information backflow is widely discussed. However, it is not easy to characterize the information flux for a given system state and show its connection to non-Markovianity. Here, by using the concepts from thermodynamics and information theory, we discuss a potential definition of information flux of an open quantum system, valid for static environments. We present a simple protocol to show how a system attempts to share information with its environment and how it builds up system-environment correlations. We also show that the information returned from the correlations characterizes the non-Markovianity and a hierarchy of indivisibility of the system dynamics.
We derive a thermodynamic uncertainty relation for work in an open quantum system driven by a time-dependent protocol and subject to repeated projective energy measurements. The protocol is represented by a sequence of protocol quenches separated by finite-time Lindblad evolution, so that work is accumulated at the quenches while dissipation occurs between them. The resulting work statistics obey the Gallavotti-Cohen symmetry to give rise to the Crooks and Jarzynski fluctuation relations. By perturbing the dissipative dynamics and combining the Cramér--Rao inequality with the quantum Fisher information, we obtain Var W/[τ∂τ⟨W⟩]2≥1/F≥max⁡(1/A,2/E)\mathrm{Var}\,W/[τ\partial_τ\langle W\rangle]^2\ge 1/F\ge\max(1/A,2/E)VarW/[τ∂τ​⟨W⟩]2≥1/F≥max(1/A,2/E), where ⟨W⟩\langle W\rangle⟨W⟩ is the work expectation value, Var W\mathrm{Var}\,WVarW is the variance of work, FFF is the Fisher information, AAA is the dynamical activity, EEE is the dimensionless entropy production, and τττ is the switching time interval between quenches. The two thermodynamic bounds follow from two independent perturbations that generate the same response of the work statistics. We illustrate the relation for a dissipative two-level system under square-wave and sinusoidal driving and show that the tighter thermodynamic bound can depend on the driving protocol and switching time scale.