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Atomic Structure, Dynamics, Changes in Chemical Bonding and Semiconductor-Metal Transition in Sb 2 Se 3 : A Remarkable Material for Quantum Networks and Energy Applications

Antimony sesquiselenide has become an outstanding functional material for photovoltaics, energy storage and transformation, memory and photonic applications. Sb 2 Se 3 is one of the most successful emerging solar light absorbers and has also been identified as a highly promising ultralow-loss phase-change material (PCM) for next-generation coherent nanophotonic processors, photonic tensor cores, quantum and neuromorphic networks. Unlike benchmark telluride PCMs, Sb 2 Se 3 features a quasi-one-dimensional (1D) crystalline structure consisting of (Sb 4 Se 6 ) ∞ ribbons, lacks the typical PCM chemical bonding, and undergoes an extended semiconductor-metal transition above the melting point. Consequently, the origin of high optical contrast between crystalline (SET) and amorphous (RESET) logic states remains elusive and presents a significant challenge. Using high-energy X-ray diffraction and Raman spectroscopy over a wide temperature range, supported by first-principles simulations and complemented by thermal, optical and electrical measurements, as well as by 121 Sb-Mossbauer spectroscopy, the quasi-1D network of orthorhombic antimony sesquiselenide was found to undergo significant evolution in amorphous and supercooled Sb 2 Se 3 , leading to lower coordination, shorter interatomic distances and a higher p-electron density on antimony, indicating changes in chemical bonding. The observed novel Sb 2 Se 3 nanocrystalline polymorph, characterized by trigonal antimony coordination and more isolated Sb-Se ribbons, could help reduce multiple trapping defect states in the bandgap, which are typical of orthorhombic Sb 2 Se 3 , thereby enhancing the power-conversion efficiency of photovoltaic devices. Semimetallic and metallic liquid Sb 2 Se 3 exhibit a gradual transformation into a denser 2D and/or 3D network with higher antimony coordination. Localized electron states in the pseudogap are becoming extended, leading to an increase in electronic conductivity σ following the relationship σ ∝ N(E F ) 2 . Liquid Sb 2 Se 3 also appears to be strongly fragile, with a nonmonotonic change in viscosity and higher atomic mobility in the metallic liquid. Furthermore, these results explain extraordinary functionalities of Sb 2 Se 3 for photonic and energy applications.

antimony↗

Materials Data on Sb2Se3 by Materials Project

Sb2Se3 is Stibnite structured and crystallizes in the orthorhombic Pnma space group. The structure is two-dimensional and consists of two Sb2Se3 sheets oriented in the (0, 0, 1) direction. there are two inequivalent Sb3+ sites. In the first Sb3+ site, Sb3+ is bonded to five Se2- atoms to form SbSe5 square pyramids that share corners with two equivalent SbSe6 octahedra, edges with three equivalent SbSe6 octahedra, and edges with four equivalent SbSe5 square pyramids. The corner-sharing octahedral tilt angles are 5°. There are a spread of Sb–Se bond distances ranging from 2.62–3.04 Å. In the second Sb3+ site, Sb3+ is bonded to six Se2- atoms to form distorted SbSe6 octahedra that share corners with two equivalent SbSe5 square pyramids, edges with four equivalent SbSe6 octahedra, and edges with three equivalent SbSe5 square pyramids. There are a spread of Sb–Se bond distances ranging from 2.71–3.25 Å. There are three inequivalent Se2- sites. In the first Se2- site, Se2- is bonded to five Sb3+ atoms to form distorted edge-sharing SeSb5 square pyramids. In the second Se2- site, Se2- is bonded in a 3-coordinate geometry to three Sb3+ atoms. In the third Se2- site, Se2- is bonded in a 2-coordinate geometry to three equivalent Sb3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Sb2Se3 by Materials Project

Sb2Se3 crystallizes in the orthorhombic Pnma space group. The structure is one-dimensional and consists of four Sb2Se3 ribbons oriented in the (1, 0, 0) direction. there are two inequivalent Sb3+ sites. In the first Sb3+ site, Sb3+ is bonded in a distorted T-shaped geometry to three Se2- atoms. There are one shorter (2.57 Å) and two longer (2.65 Å) Sb–Se bond lengths. In the second Sb3+ site, Sb3+ is bonded in a distorted T-shaped geometry to three Se2- atoms. There are one shorter (2.62 Å) and two longer (2.63 Å) Sb–Se bond lengths. There are three inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in an L-shaped geometry to two equivalent Sb3+ atoms. In the second Se2- site, Se2- is bonded in an L-shaped geometry to two Sb3+ atoms. In the third Se2- site, Se2- is bonded in an L-shaped geometry to two equivalent Sb3+ atoms.

36 MATERIALS SCIENCE↗