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

Statistical mechanics of a quantum fluid near T = 0

James R. Henderson

Published Nov 1, 1982• 0 citations
Publisher
DOI
10.1016/0378-4371(82)90246-1

Related papers

Equilibrium statistical mechanics of quantum fluids

Bijoy Kumar

•Jan 1, 1968•0 citations

Quantum Statistical Theory of the Degenerate Bose Fluid

Dion W. J. Shea

•Jan 1, 1969•0 citations

Dynamical Indistinguishability and Statistics in Quantum Fluids

Kostya Trachenko, Alessio Zaccone

•Jan 1, 2022•0 citations

(ħ, k)-Dynamics as some generalization of equilibrium quantum statistical mechanics

Alexander D. Sukhanov, O. N. Golubjeva

We show that the quantum statistical mechanics (QSM) describing quantum and thermal properties of objects has only the sense of a particular semiclassical approximation. We propose a more general (than QSM) micro description of objects in a heat bath taken into account a vacuum as an object environment; we call it ( ħ, k )-dynamics ( ħkD ). We construct a new model of thermostat, namely, a quantum heat bath and study its properties including the cases of a “cold” and “thermal” vacua. We introduce a new generative operator, Schroedingerian, or stochastic action operator, and show its fundamental role in the determination such macro-quantities as internal energy, effective temperature, and effective entropy. We establish that in ħkD the ratio of effective action to effective entropy at zero temperature equals the universal constant ħ /2 k . This result corresponds to experimental data taken recently under studying of a new matter state—nearly perfect fluid.

Physics of Particles and Nuclei•Nov 25, 2010•0 citations

A Lattice Model of a Quantum Fluid

Donald D. Betts, D. Cuthiell

Elsevier eBooks•Jan 1, 1980•0 citations

New version of quantum mechanics at finite temperatures as a ground for description of nearly perfect fluids

Alexander D. Sukhanov, O. N. Golubjeva

We suggest a more general than quantum statistical mechanics ($QSM$) microdescription of objects in a heat bath taken into account a vacuum as an object environment - modification of quantum mechanics at finite temperatures; we call it $(\hbar, k)$-dynamics ($ \hbar kD$). This approach allows us in a new manner to calculate some important macroparameters and to modify standard thermodynamics. We create an effective apparatus for features description of nearly perfect fluids in various mediums. As an essentially new model of an object environment we suppose a quantum heat bath and its properties, including cases of cold and warm vacuums, are studied. We describe the thermal equilibrium state in place of the traditional density operator in term of a wave function the amplitude and phase of which have temperature dependence. We introduce a new generative operator, Schroedingerian, or stochastic action operator, and show its fundamental role in the microdescription. We demonstrate that a new macroparameter, namely the effective action, can be obtained through averaging of the Schroedingerian over the temperature dependent wave function. It is established that such different parameters as internal energy, effective temperature, and effective entropy and their fluctuations can be expressed through a single quantity - the effective action.

arXiv:1012.5056•Dec 22, 2010•0 citations
We show that the quantum statistical mechanics (QSM) describing quantum and thermal properties of objects has only the sense of a particular semiclassical approximation. We propose a more general (than QSM) micro description of objects in a heat bath taken into account a vacuum as an object environment; we call it ( ħ, k )-dynamics ( ħkD ). We construct a new model of thermostat, namely, a quantum heat bath and study its properties including the cases of a “cold” and “thermal” vacua. We introduce a new generative operator, Schroedingerian, or stochastic action operator, and show its fundamental role in the determination such macro-quantities as internal energy, effective temperature, and effective entropy. We establish that in ħkD the ratio of effective action to effective entropy at zero temperature equals the universal constant ħ /2 k . This result corresponds to experimental data taken recently under studying of a new matter state—nearly perfect fluid.
We suggest a more general than quantum statistical mechanics (QSMQSMQSM) microdescription of objects in a heat bath taken into account a vacuum as an object environment - modification of quantum mechanics at finite temperatures; we call it (ℏ,k)(\hbar, k)(ℏ,k)-dynamics ($ \hbar kD$). This approach allows us in a new manner to calculate some important macroparameters and to modify standard thermodynamics. We create an effective apparatus for features description of nearly perfect fluids in various mediums. As an essentially new model of an object environment we suppose a quantum heat bath and its properties, including cases of cold and warm vacuums, are studied. We describe the thermal equilibrium state in place of the traditional density operator in term of a wave function the amplitude and phase of which have temperature dependence. We introduce a new generative operator, Schroedingerian, or stochastic action operator, and show its fundamental role in the microdescription. We demonstrate that a new macroparameter, namely the effective action, can be obtained through averaging of the Schroedingerian over the temperature dependent wave function. It is established that such different parameters as internal energy, effective temperature, and effective entropy and their fluctuations can be expressed through a single quantity - the effective action.