Mézard and Parisi recently proposed a method for investigating the thermodynamics of a supercooled liquid around and below its glass transition. This approach assumes the existence of a true phase transition at a (finite) Kauzmann temperature TK, which is determined, and gives a quantitative estimate of the jump of specific heat ΔCv at TK. Using the simplest possible scheme, we apply this formalism to a system of pure “soft-spheres” fluid, when the dimension d of the embedding space is lower than 3 (and possibly noninteger). Looking for a lower critical dimension (which we do not find), we assess the mean-field character of the approximation used in the above mentioned approach.
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Fabrice Thalmann (2002) studied this question.
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