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

The European Physical Journal Special Topics

Nonequilibrium quantum stochastic thermodynamics for bosons and fermions

Tânia Tomé, Mário J. de Oliveira

Published Apr 5, 2023• 2 citations
Publisher
DOI
10.1140/epjs/s11734-023-00802-y

Related papers

Application of the method of nonequilibrium thermodynamic potentials to systems of fermions interacting with bosons

A. P. Grigin, É.L. Nagaev

Theoretical and Mathematical Physics•Mar 1, 1974•2 citations

Nonequilibrium temperature for open boson and fermion systems

Sang Pyo Kim

•Jan 1, 2002•2 citations

Bosonic and fermionic descriptions for a simple nonequilibrium model

Carlos E. Fiore, Juan A. Bonachela, Miguel A. Muñoz

AIP conference proceedings•Jan 1, 2007•0 citations

Quantum stochastic differential equations for boson and fermion systems—method of non-equilibrium thermo field dynamics

A.E. Kobryn, T. Hayashi, T. Arimitsu

arXiv:math-ph/0304023•Annals of Physics•Sep 16, 2003•10 citations

Nonequilibrium entropic temperature and its lower bound for quantum stochastic processes

Somrita Ray, Alendu Baura, Bidhan Chandra Bag

In this paper, we have studied the Shannon "entropic" nonequilibrium temperature (NET) of quantum Brownian systems. The Brownian particle is attached to either a bosonic or fermionic bath. Based on the Fokker-Planck description of the c-number quantum Langevin equation, we have calculated entropy production, NET, and their bounds. Entropy production (EP), the upper bound of entropy production (UBEP), and the deviation of the UBEP from EP monotonically decrease as functions of time to equilibrium value for both of the thermal baths. The deviation decreases with increase of temperature of the bosonic thermal bath, but it becomes larger as the temperature of the fermionic bath grows. We also observe that nonequilibrium temperature and its lower bound monotonically increase to equilibrium value with the progression of time. But their difference as a function of time shows an optimum behavior in most cases. Finally, we have observed that at long time, the entropic temperature (for a bosonic thermal bath) first increases nonlinearly as a function of thermodynamic temperature (TT) and, if the TT is appreciably large, then it grows linearly. But for the fermionic thermal bath, the entropic temperature decreases monotonically as a nonlinear function of thermodynamic temperature to zero value.

Physical Review E•Mar 31, 2014•5 citations

Quantum Stochastic Systems in Terms of Non-Equilibrium Thermo Field Dynamics

Toshihico Arimitsu, Takeshi Saito, T. Imagire

Springer eBooks•Jan 1, 1997•0 citations
In this paper, we have studied the Shannon "entropic" nonequilibrium temperature (NET) of quantum Brownian systems. The Brownian particle is attached to either a bosonic or fermionic bath. Based on the Fokker-Planck description of the c-number quantum Langevin equation, we have calculated entropy production, NET, and their bounds. Entropy production (EP), the upper bound of entropy production (UBEP), and the deviation of the UBEP from EP monotonically decrease as functions of time to equilibrium value for both of the thermal baths. The deviation decreases with increase of temperature of the bosonic thermal bath, but it becomes larger as the temperature of the fermionic bath grows. We also observe that nonequilibrium temperature and its lower bound monotonically increase to equilibrium value with the progression of time. But their difference as a function of time shows an optimum behavior in most cases. Finally, we have observed that at long time, the entropic temperature (for a bosonic thermal bath) first increases nonlinearly as a function of thermodynamic temperature (TT) and, if the TT is appreciably large, then it grows linearly. But for the fermionic thermal bath, the entropic temperature decreases monotonically as a nonlinear function of thermodynamic temperature to zero value.