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Materials Data on Ag(AuS)2 by Materials Project

Ag(AuS)2 crystallizes in the monoclinic Pc space group. The structure is three-dimensional. there are two inequivalent Au+1.50+ sites. In the first Au+1.50+ site, Au+1.50+ is bonded in a distorted linear geometry to two S2- atoms. There are one shorter (2.32 Å) and one longer (2.34 Å) Au–S bond lengths. In the second Au+1.50+ site, Au+1.50+ is bonded in a linear geometry to two equivalent S2- atoms. Both Au–S bond lengths are 2.33 Å. Ag1+ is bonded in a 4-coordinate geometry to four S2- atoms. There are a spread of Ag–S bond distances ranging from 2.50–2.97 Å. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to three Au+1.50+ and one Ag1+ atom to form distorted corner-sharing SAgAu3 tetrahedra. In the second S2- site, S2- is bonded in a 4-coordinate geometry to one Au+1.50+ and three equivalent Ag1+ atoms.

36 MATERIALS SCIENCE↗

Transport and optical properties of the chiral semiconductor Ag 3 AuSe 2

Previous band structure calculations predicted Ag 3 AuSe 2 to be a semiconductor with a band gap of approximately 1 eV. Here, we report single crystal growth of Ag 3 AuSe 2 and its transport and optical properties. Single crystals of Ag 3 AuSe 2 were synthesized by slow-cooling from the melt, and grain sizes were confirmed to be greater than 2 mm using electron backscatter diffraction. Optical and transport measurements reveal that Ag 3 AuSe 2 is a highly resistive semiconductor with a band gap and activation energy around 0.3 eV. Our first-principles calculations show that the experimentally determined band gap lies between the predicted band gaps from GGA and hybrid functionals. We predict band inversion to be possible by applying tensile strain. The sensitivity of the gap to Ag/Au ordering, chemical substitution, and heat treatment merit further investigation.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗