The viscosity data measured by penetration and parallelāplate methods for As2Se3 glass and undercooled melt were compared with literature data. The MYEGA equation (log Ī·0Ā =Ā ā4.67Ā Ā±Ā 0.12, mĀ =Ā 43.2Ā Ā±Ā 0.4, and T12Ā =Ā 441.7Ā Ā±Ā 0.3 K) was used for the description of the selected viscosity data, including melt region (15 orders of magnitude). The heat capacity data for As2Se3 glass, undercooled melt, and melt, as well as for crystalline As2Se3 were determined for low and mediumārange temperature intervals. These data were compared with previously reported data. Equations that describe the heat capacity of As2Se3 in a broad temperature interval were formulated. The values of the standard molar enthalpy, Ī0THm0, and entropy, Ī0TSm0, at TĀ =Ā 298.15 K are 26.202Ā kJĀ·molā1 and 193.8 JĀ·molā1Ā·Kā1, respectively. The heat capacity data determined from very low temperatures were used for the calculation of crystal, glass, and melt entropies. These heat capacity temperature dependencies were used both for the estimation of the Kauzmann temperature (TKĀ =Ā 292.5 K) and the glass entropy at 0 K (S0Ā =Ā 25.96 JĀ·molā1Ā·Kā1), and for the determination of the excess entropy. The proportionality between the viscosity of the As2Se3 melt and the excess entropy clearly indicates the applicability of the AdamāGibbs (AG) model.