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

Thermodynamic properties of the low-dimensional perfect Bose gas

Gaetano Busiello, L. De Cesare, Dimo I. Uzunov

Published Aug 1, 1985• 6 citations
Publisher
DOI
10.1016/0378-4371(85)90125-6

Related papers

Thermodynamic Properties of the Weakly Interacting Bose System

K. Matsuda

芝浦工業大学研究報告 理工系編•Mar 1, 2000•0 citations

Thermodynamics of a dilute non-perfect Bose-Einstein gas

Yves Pomeau A, Sergio Rica

We study the thermodynamics of a dilute Bose gas. Not too close to the Bose-Einstein transition we find results differing from the ones in the literature. As a consequence the low momentum part of the distribution of quasiparticules is not a Bose factor, and the effective spectrum is not of the phonon type. We also discuss the possibility of a Bose-Einstein transition in 2 D .

Europhysics Letters (EPL)•Jul 1, 2000•5 citations

Optical probes of coherence in two-dimensional Bose gases of polaritons

Joseph Jachinowski, Hassan Alnatah, David W. Snoke +1 more

Due to their photonic components, exciton-polariton systems provide a convenient platform to study the coherence properties of weakly-interacting Bose gases. In particular, optical interferometry enables the measurement of the first-order coherence function which provides information about the intrinsic correlations of the system. In this paper, we derive a universal curve for the coherent fraction of a noninteracting, equilibrium, homogeneous, two-dimensional Bose gas, with density expressed in units of the observation area, and compare to recent experimental results. Although there is a sharp transition from normal to superfluid phases in the thermodynamic limit, the coherent fraction of the gas varies continuously across this transition due to the finite system size. We find that the theory agrees nearly perfectly with the experimental data in the low-density limit with no free parameters other than the effective temperature, highly constrained by the measurements. At higher density, the experiments are consistent with standard weakly-interacting Bose gas theory. By having a theory that treats both the optical diffraction and Bose coherence, we can clearly see the effect of the quantum statistics on the coherence.

arXiv:2503.08629•Physical Review A•Jun 15, 2026•0 citations

Thermodynamics of a one-dimensional lattice Bose gas

N. M. Bogoliubov

Theoretical and Mathematical Physics•Jun 1, 1986•1 citation

ON THE THERMODYNAMICS OF THE BOSE GAS

Yu.B. Rumer

Zhur. Eksptl'. i Teoret. Fiz.•Sep 1, 1950•0 citations

The properties of a perfect Einstein-Bose gas at low temperatures

R. H. Fowler, Hilary D. Jones

In a recent letter to Nature F. London(3) has called attention to a discontinuity in the derivative dCV/dT of the specific heat with respect to temperature which arises in a perfect Einstein-Bose gas at low temperatures. When discussing the properties of a perfect gas satisfying the Bose statistics, Einstein(1) remarked that at low temperatures something resembling a condensed phase should appear. The temperature at which this condensation should begin is given by the equation where n is the number of particles of mass m per unit volume and the other symbols have their usual significance.

Mathematical Proceedings of the Cambridge Philosophical Society•Oct 1, 1938•21 citations
Due to their photonic components, exciton-polariton systems provide a convenient platform to study the coherence properties of weakly-interacting Bose gases. In particular, optical interferometry enables the measurement of the first-order coherence function which provides information about the intrinsic correlations of the system. In this paper, we derive a universal curve for the coherent fraction of a noninteracting, equilibrium, homogeneous, two-dimensional Bose gas, with density expressed in units of the observation area, and compare to recent experimental results. Although there is a sharp transition from normal to superfluid phases in the thermodynamic limit, the coherent fraction of the gas varies continuously across this transition due to the finite system size. We find that the theory agrees nearly perfectly with the experimental data in the low-density limit with no free parameters other than the effective temperature, highly constrained by the measurements. At higher density, the experiments are consistent with standard weakly-interacting Bose gas theory. By having a theory that treats both the optical diffraction and Bose coherence, we can clearly see the effect of the quantum statistics on the coherence.
In a recent letter to Nature F. London(3) has called attention to a discontinuity in the derivative dCV/dT of the specific heat with respect to temperature which arises in a perfect Einstein-Bose gas at low temperatures. When discussing the properties of a perfect gas satisfying the Bose statistics, Einstein(1) remarked that at low temperatures something resembling a condensed phase should appear. The temperature at which this condensation should begin is given by the equation where n is the number of particles of mass m per unit volume and the other symbols have their usual significance.