1. Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA

Correspondence to: C. A. Angell Correspondence and requests for materials should be addressed to C.A.A. (e-mail: Email: caa@asu.edu).

Abstract

Although liquids normally crystallize on cooling, there are members of all liquid types (including molecular, ionic and metallic) that supercool and then solidify at their glass transition temperature, T_g. This continuous solidification process exhibits great diversity within each class of liquid—both in the steepness of the viscosity–temperature profile, and in the rate at which the excess entropy of the liquid over the crystalline phase changes as T_g is approached. However, the source of the diversity is unknown. The viscosity and associated relaxation time behaviour have been classified between 'strong' and 'fragile' extremes, using T_g as a scaling parameter¹, but attempts to correlate such kinetic properties with the thermodynamic behaviour have been controversial^{2, 3}. Here we show that the kinetic fragility can be correlated with a scaled quantity representing excess entropy, using data over the entire fragility range and embracing liquids of all classes. The excess entropy used in our correlation contains both configurational and vibration-related contributions. In order to reconcile our correlation with existing theory and simulations, we propose that variations in the fragility of liquids originate in differences between their vibrational heat capacities, harmonic and anharmonic, which we interpret in terms of an energy landscape. The differences evidently relate to behaviour of low-energy modes near and below the boson peak.