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

Physica A Statistical Mechanics and its Applications

On the kinetics of subsystems interacting with Bosons

Victor F. Los, A.G. Martynenko

Published Oct 1, 1986• 3 citations
Publisher
DOI
10.1016/0378-4371(86)90031-2

Related papers

Nonlinear feedback effects in coupled boson-fermion systems

T. Domański, J. Ranninger

We address ourselves to a class of systems composed of two coupled subsystems without any intrasubsystem interaction: itinerant fermions and localized bosons on a lattice. Switching on an interaction between the two subsystems leads to feedback effects which result in a rich dynamical structure in both of them. Such feedback features are studied on the basis of the flow equation technique---an infinite series of infinitesimal unitary transformations---which leads to a gradual elimination of the intersubsystem interaction. As a result the two subsystems get decoupled but their renormalized kinetic energies become mutually dependent on each other. Choosing for the intersubsystem interaction a charge exchange term,---the boson-fermion model---the initially localized bosons acquire itinerancy through their dependence on the renormalized fermion dispersion. This latter evolves from a free particle dispersion into one showing a pseudogap structure near the chemical potential. Upon lowering the temperature both subsystems simultaneously enter a macroscopic coherent quantum state. The bosons become superfluid, exhibiting a soundwavelike dispersion while the fermions develop a true gap in their dispersion. The essential physical features described by this technique are already contained in the renormalization of the kinetic terms in the respective Hamiltonians of the two subsystems. The extra interaction terms resulting in the process of iteration only strengthen this physics. We compare the results with previous calculations based on self-consistent perturbative approaches.

arXiv:cond-mat/0012081•Physical review. B, Condensed matter•Mar 1, 2001•55 citations

Some consequences of kinetic theory for bosons

German A. Skorobogatov, B.E. Dzevitskii

Soviet physics. Doklady•Apr 1, 1974•0 citations

Reduction of a Boson Subsystem up to the Lowest Order

Toshihico Arimitsu

Derivation of a master equation is given in the case where a Boson subsystem can be eliminated besides reservoirs by using the time-convolution-less formulation of the damping theory within the conventional treatment, up to the lowest order expansion of the “kinetic coefficient” with respect to the coupling constant between the Boson subsystem and the remaining ones. Useful diagramatic expansion of Liouville operators, formula for the elimination of Boson operators and algebraic formulae of the spin coherent representation are given in Appendices.

Journal of the Physical Society of Japan•Feb 1, 1982•7 citations

Complex Dynamics in Systems of Interacting Bosons

Moritz Hiller, Joshua D. Bodyfelt, Tsampikos Kottos +1 more

APS•Mar 1, 2007•0 citations

Kinetic theory for quantum nanosystems

Massimiliano Esposito

In this thesis, we investigate the emergence of kinetic processes in finite quantum systems. We first generalize the Redfield theory to describe the dynamics of a small quantum system weakly interacting with an environment of finite heat capacity. We then study in detail the spin-GORM model, a model made of a two-level system interacting with a random matrix environment. By doing this, we verify our new theory and find a critical size of the environment over which kinetic processes occur. We finally study the emergence of a diffusive transport process, on a finite tight-binding subsystem interacting with a fast environment, when the size of subsystem exceeds a critical value.

arXiv:cond-mat/0412495•Dec 17, 2004•0 citations

On the microscopic theory of interacting bosons

Peter A. Ring, Y. K. Gambhir, S. Iwasaki +1 more

Progress in Particle and Nuclear Physics•Jan 1, 1983•1 citation
We address ourselves to a class of systems composed of two coupled subsystems without any intrasubsystem interaction: itinerant fermions and localized bosons on a lattice. Switching on an interaction between the two subsystems leads to feedback effects which result in a rich dynamical structure in both of them. Such feedback features are studied on the basis of the flow equation technique---an infinite series of infinitesimal unitary transformations---which leads to a gradual elimination of the intersubsystem interaction. As a result the two subsystems get decoupled but their renormalized kinetic energies become mutually dependent on each other. Choosing for the intersubsystem interaction a charge exchange term,---the boson-fermion model---the initially localized bosons acquire itinerancy through their dependence on the renormalized fermion dispersion. This latter evolves from a free particle dispersion into one showing a pseudogap structure near the chemical potential. Upon lowering the temperature both subsystems simultaneously enter a macroscopic coherent quantum state. The bosons become superfluid, exhibiting a soundwavelike dispersion while the fermions develop a true gap in their dispersion. The essential physical features described by this technique are already contained in the renormalization of the kinetic terms in the respective Hamiltonians of the two subsystems. The extra interaction terms resulting in the process of iteration only strengthen this physics. We compare the results with previous calculations based on self-consistent perturbative approaches.
Derivation of a master equation is given in the case where a Boson subsystem can be eliminated besides reservoirs by using the time-convolution-less formulation of the damping theory within the conventional treatment, up to the lowest order expansion of the “kinetic coefficient” with respect to the coupling constant between the Boson subsystem and the remaining ones. Useful diagramatic expansion of Liouville operators, formula for the elimination of Boson operators and algebraic formulae of the spin coherent representation are given in Appendices.
In this thesis, we investigate the emergence of kinetic processes in finite quantum systems. We first generalize the Redfield theory to describe the dynamics of a small quantum system weakly interacting with an environment of finite heat capacity. We then study in detail the spin-GORM model, a model made of a two-level system interacting with a random matrix environment. By doing this, we verify our new theory and find a critical size of the environment over which kinetic processes occur. We finally study the emergence of a diffusive transport process, on a finite tight-binding subsystem interacting with a fast environment, when the size of subsystem exceeds a critical value.