Supercooled liquids, glass transitions, and the Kauzmann paradox

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Abstract
Many liquids have heat capacities that substantially exceed those of the corresponding crystal, and this discrepancy magnifies in the supercooled regime. Thus, liquidentropy declines more rapidly with temperature than does crystal entropy, and the former paradoxically seems to fall below the latter for temperatures below the Kauzmann point T K . Although laboratory glass transitions inevitably intervene to prevent observation of this entropy crossing, it has often been argued that a second‐order ‘‘ideal glass transition’’ in principle should occur at T K . The inherent structure theory of condensed phases has been modified to describe supercooled liquids, and has been applied to this Kauzmann paradox. The conclusion is that an ideal glass transition of the type normally associated with the Kauzmann phenomenon cannot occur for substances of limited molecular weight and with conventional intermolecular interactions. This result also subverts theoretical expressions for shear viscosity (such as the Tamman–Vogel–Fulcher and the mode‐coupling formulas) that diverge to infinity at an ideal glass transition temperature.