Antimony chalcogenides

Sb₂Se₃, Sb₂S₃; the bismuth analogue Bi₂S₃

Also called Sb₂Se₃, Sb₂S₃, Bi₂S₃, antimony selenide

van der Waals crystal semiconductor

The solar absorber that is van der Waals in one direction. Sb2Se3 is built from covalent ribbons that only touch each other weakly, so a grain boundary between two aligned ribbons has no dangling bonds to trap carriers – the reason these films tolerate the kind of polycrystalline growth that ruins most absorbers. The compounds are binary, cheap, non-toxic and stable, and the same weak bonding that helps the solar cells also makes Sb2S3 and Sb2Se3 the lowest-loss phase-change materials for programmable photonic chips.

Key properties

  • Quasi-one-dimensional structure: strong bonds along the ribbon, van der Waals bonds between ribbons, so properties depend strongly on ribbon orientation
  • Benign grain boundaries when ribbons are aligned along the growth direction – the guiding idea behind Sb2Se3 photovoltaics
  • Band gaps spanning the useful solar range, from ~1.2 eV in Sb2Se3 to ~1.7 eV in Sb2S3
  • Simple, stable binary compounds from earth-abundant, low-toxicity elements
  • As phase-change materials they switch with almost no optical loss: refractive-index contrast of 0.60 (Sb2S3) and 0.77 (Sb2Se3) with k below 10−5 at 1,550 nm, and thousands of switching cycles
  • That combination beats Ge2Sb2Te5 by two orders of magnitude on phase shift per decibel of loss

How it is made

  • Thin films by close-space sublimation, vapour transport deposition, chemical bath deposition or evaporation – the routes used for solar cells
  • Bulk crystals and nanoribbons from melt or solution growth; the ribbons can be dispersed but are rarely exfoliated as sheets
  • Growth is tuned to orient the ribbons across the film, because misaligned ribbons leave carriers to cross weakly bonded boundaries

Uses, and how close they are

  • Thin-film solar absorbers (Sb2Se3, Sb2S3)prototype
  • Low-loss phase-change materials for programmable photonicslab
  • Photodetectors and photoelectrochemical electrodeslab

Readiness runs lab → prototype → pilot → deployed.

Open problems

  1. How far can ribbon alignment be controlled across a full film, and what happens at the boundaries that are not aligned?
  2. What limits the open-circuit voltage – bulk defects, band tails, or the interfaces with the contact layers?
  3. Can doping be controlled deliberately, rather than through selenium stoichiometry?
  4. Do single ribbons or thin flakes behave like the bulk, and is there a device case for isolating them?

Going deeper

Short notes for specialists. Choose a lens in the header and yours comes first.

For theoreticians · your lens

A quasi-one-dimensional crystal in three dimensions: within a ribbon the bonding is covalent, between ribbons it is dispersion-dominated, so calculations need van der Waals corrections and an anisotropic effective mass that differs by a factor of several between along-ribbon and cross-ribbon directions. The much-cited claim that grain boundaries are benign rests on surfaces of aligned ribbons having no dangling bonds, which makes defect calculations at realistic boundaries the interesting test. Native defects – antimony and selenium vacancies and antisites – set the doping and the band tails that limit open-circuit voltage.

For experimentalists · your lens

Orientation is the measurement that matters: X-ray diffraction texture, specifically how much of the film grows with ribbons pointing out of the plane, predicts device performance better than grain size does. Report the deposition route and substrate temperature together, since they set that texture. For phase-change work, quote the crystalline and amorphous refractive indices and the loss at the operating wavelength, and count switching cycles rather than single-shot contrast.

For engineers · your lens

Cheap, stable, binary and non-toxic, with a band gap close to ideal for single-junction cells – but solar efficiencies remain far behind CdTe and CIGS, and the open-circuit voltage is the gap. In photonics the case is stronger: Sb2Se3 and Sb2S3 switch with so little absorption that they make practical programmable waveguides, where the established phase-change alloys lose too much light.

Recent news

The newest items tagged Sb2Se3, Sb2S3, from the news feed updated 5 Oct 2026.

Preprintnot yet peer reviewed arXiv

Numerical exploration on unveiling the photovoltaic potential of MgXS3(X = Ti, Zr, Hf) chalcogenide perovskites

Lead-free chalcogenide perovskites offer a nontoxic and thermally robust path beyond Pb-based perovskite solar cells (PSCs), but their device-level behavior in realistic three-dimensional geometries remains insufficiently characterized. In this work, we investigate ZnSe/MgXS3(X = Ti, Zr, Hf)/Sb2S3 solar cell…

ExperimentEngineeringSb₂Se₃, Sb₂S₃
Preprintnot yet peer reviewed arXiv

Low loss switchable topological photonic crystal enabled by submicron-scale patterning and phase-change of Sb2Se3

Photonic topological insulators (PTIs) offer robust platforms for light manipulation, but reconfigurable control of their topological properties without degrading performance remains a major challenge. While phase-change materials (PCMs) provide large refractive index modulation, widely used materials such as Ge2Sb2Te5…

Preprintnot yet peer reviewed arXiv

Amplified Directional Photoluminescence from CIS Quantum Dots and hBN Quantum Emitters using Tunable BIC Metasurfaces

Integrated and tunable light sources are critical for advancing quantum nanophotonic chips in quantum computing, communications, and sensing. However, efficient and tunable emission amplification post-fabrication poses major challenges. Hybrid metasurfaces combining niobium pentoxide (Nb2O5), copper indium sulfide…

All 4 items tagged Sb₂Se₃, Sb₂S₃ in the news feed  ·  RSS feed for Sb₂Se₃, Sb₂S₃

Key references

  1. Thin-film Sb2Se3 photovoltaics with oriented one-dimensional ribbons and benign grain boundariesZhou et al. · Nature Photonics 9, 409 (2015)cited by 1,046doi:10.1038/nphoton.2015.78
  2. Characterization of basic physical properties of Sb2Se3 and its relevance for photovoltaicsChen et al. · Frontiers of Optoelectronics 10, 18 (2017)cited by 424doi:10.1007/s12200-017-0702-z
  3. A new family of ultralow loss reversible phase-change materials for photonic integrated circuits: Sb2S3 and Sb2Se3Delaney et al. · Advanced Functional Materials 30, 2002447 (2020)cited by 673doi:10.1002/adfm.202002447