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Bose-Einstein condensation in layered systems

A Haerdig and F Ravndal

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The thermodynamic properties of an ideal gas of bosons moving freely within layered planes and having a finite amplitude for jumping between neighbouring planes, are derived. As long as this coupling is non-zero, the system becomes effectively two-dimensional at sufficiently high temperatures. At a correspondingly low temperature it undergoes a Bose-Einstein transition into a condensed phase as in three dimensions. Below the critical temperature the specific heat is a universal function of only one dimensionless system variable. The phase transition becomes weaker as the coupling between the planes decreases and eventually disappears when the planes decouple.


PACS

03.75.Hh Static properties of condensates; thermodynamical, statistical and structural properties

05.70.Fh Phase transitions: general studies

05.70.Ce Thermodynamic functions and equations of state

51.30.+i Thermodynamic properties, equations of state

Subjects

Quantum gases, liquids and solids

Plasma physics

Statistical physics and nonlinear systems

Dates

Issue 4 (July 1993)



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