Abstract

We study the Casimir effect in the vicinity of a quantum critical point. As a prototypical system we analyze the dd-dimensional imperfect (mean-field) Bose gas enclosed in a slab of extension Ld−1×DL^{d-1}\times D and subject to periodic boundary conditions. The thermodynamic state is adjusted so that L≫λ≫D≫łmicL\ggλ\gg D\ggł_{mic}, where λ∼T−1/2λ\sim T^{-1/2} is the thermal de Broglie length, and lmicl_{mic} denotes microscopic lengthscales. Our exact analysis indicates that the Casimir force in the above specified regime is generically repulsive and decays either algebraically or exponentially, with a non-universal amplitude.

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