Critical temperature shifts for finite slabs in the ε-expansion

The critical temperature Tc(b) of a d-dimensional system with finite thickness b in one of its dimensions approaches its bulk limit as b to infinity according to Tc( infinity )-Tc(b) varies as b- lambda . To first order in epsilon =4-d the shift exponent lambda is found to be given by lambda =2-((n+2)/(n+8)) epsilon +O( epsilon 2), and thus satisfies the scaling relation lambda = nu d-1, where nu d is the correlation length exponent of the bulk system and n is the order parameter dimensionality.

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