Abstract
Abstract
We present an analytically solvable theory of Bose–Einstein condensation (BEC) in thin film geometries. Analytical closed-form expressions for the critical temperature are obtained in both the low-to-moderate confinement regime (where the film thickness L is in the order of microns) as well as in the strong confinement regime where the thickness is in the order of few nanometers or lower. The possibility of high-temperature BEC is predicted in the strong confinement limit, with a square-root divergence of the critical temperature T
c ∼ L
−1/2. For cold Bose gases, this implies an enhancement up to two orders of magnitude in T
c for films on the nanometer scale. Analytical predictions are also obtained for the heat capacity and the condensate fraction. A new law for the heat capacity of the condensate, i.e. C ∼ T
2, is predicted for nano-scale films, which implies a different λ-point behavior with respect to bulk systems, while the condensate fraction is predicted to follow a
[
1
−
(
T
/
T
c
)
2
]
law.
Subject
Condensed Matter Physics,Atomic and Molecular Physics, and Optics
Cited by
4 articles.
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