The As 2 S 3 melt at room pressure represents a liquid having a three-dimensional network structure, semiconducting properties, and a huge viscosity. We have found that under high pressure a considerable change in the medium and short-range structure of this liquid is observed. Intermediate-range order correlations in the atomic arrangement almost disappear under pressure and an increase in the coordination number is observed. This increase is evidently associated with the formation of a significant fraction of the wrong neighbors As-As. At pressures above 6 GPa, the As 2 S 3 melt has a conductivity close to the minimum conductivity value of ϳ100 Ohm −1 cm −1 and a moderate viscosity of ϳ0.5-1 Pa s. Obviously, the transition under high pressures to such "strange metallic" liquids are bound to be seen in many other chalcogenide melts with network structure.Phase transformations in liquids and a change in the structure and properties of liquids under pressure are one of the hottest topics of condensed-matter physics. 1,2 The As 2 S 3 melt is one of the most important archetypical strong glassforming liquids, whose viscosity of 8000 Pa s near the melting temperature at normal pressure is record high for chalcogenide melts, 3 making the crystallization of As 2 S 3 almost impossible. 4 The As 2 S 3 substance ranks first among chalcogeniges from the viewpoint of the production of amorphous and glasslike industrial materials. The crystalline phase of As 2 S 3 is a semiconductor ͑orpiment͒ with a layer structure, each As atom is surrounded by three S atoms and each S atom by two As atoms. The liquid and glassy states of As 2 S 3 largely preserve the short-range order ͑SRO͒ and mediumrange order ͑MRO͒ of the crystalline counterpart and have a similar electronic structure. 5 However, the layer structure in the melt is partially disrupted and the liquid network contains some amount of broken bonds or "wrong" As-As ͑S-S͒ bonds. 6 Interest in liquid arsenide chalcogenides, such as As 2 S 3 , As 2 Se 3 , and As 2 Te 3 , as well as in elementary liquid Se, S, and Te, is also aroused by the fact that the transition from a semiconductor to a metallic state occurs in these melts at high temperatures and moderate pressures in the supercritical region 7-12 and ͑or͒ under high pressures in the vicinity of the melting curve. [13][14][15][16][17] Similarly, the glassy states of these materials undergo a semiconductor-metal transition under compression at room temperature. 18 The mechanism of the semiconductor-metal transition in these substances has not yet been fully clarified; 7 at any case, it is not the classical Mott-type transition. 5 The best theoretically and experimentally studied semiconductor-metal transition is the one occurring in liquid chalcogenides As 2 Se 3 , As 2 S 3 , and As 2 Te 3 , and liquid Se at high temperatures and moderate pressures. This transition is accompanied by significant structural and thermodynamic changes. 7-12 It has been found that with an increase in temperature, the three-dimensional network str...