Rhodium chalcohalides

RhSeCl, RhTeCl; also RhSeBr and RhSeCl₀.₅Br₀.₅

Also called RhSeCl, RhTeCl, RhSeBr, rhodium chalcochlorides

van der Waals crystal semiconductor

Most Janus layers – sheets whose two faces are made of different atoms – have to be made one at a time, by replacing the atoms on one face of an existing monolayer. RhSeCl grows that way by itself: every layer of the crystal has selenium on one side and chlorine on the other, so Janus flakes can simply be peeled off a bulk crystal. The built-in asymmetry makes it a semiconductor with an unusually strong nonlinear optical response. Its sister compound RhTeCl arranges tellurium and chlorine in stripes instead, which gives needle-shaped flakes and a smaller band gap.

Crystal structure

  • Rh
  • Se
  • Cl
Cell
Hexagonal, a = 3.49 Å
Atoms per cell
3
Rh–Se bond
2.38 Å
Rh–Cl bond
2.51 Å
Height
2.77 Å between the outer atom centres
A plane of rhodium with selenium on one face and chlorine on the other; each Rh sits in an octahedron of three Se and three Cl atoms. The two faces differ, so the layer has no inversion centre, which is what allows its strong second-harmonic generation. The Rh–Cl bonds are longer than the Rh–Se bonds, so the chlorine plane sits farther from the metal. RhTeCl, the other compound on this page, mixes tellurium and chlorine in stripes on both faces instead. One layer of bulk RhSeCl at 293 K, from single-crystal X-ray diffraction (Nowak, doctoral thesis, TU Dresden, 2025): a = 3.488 Å, c = 11.579 Å. Every atom sits on a threefold axis, so the cell and the two bond lengths fix the layer completely.

Key properties

  • RhSeCl is a natural Janus crystal: every layer is polar, and the layers stack so that the bulk crystal keeps that polarity
  • Very strong second-harmonic generation in RhSeCl, with χ(2) above 3000 pm/V reported near 0.9 eV, weakening as the temperature rises
  • Both compounds are diamagnetic semiconductors
  • RhTeCl’s alternating Te and Cl stripes make its flakes needle-shaped and its properties strongly direction-dependent
  • RhSeCl has been exfoliated down to monolayers, whose Raman spectra stay close to those of the bulk crystal
  • RhSeCl is stable to about 700 °C and decomposes at 917 °C, losing its chlorine; RhTeCl is stable only to about 600 °C and decomposes at 761 °C, losing its chlorine and about half its tellurium
  • Replacing half the chlorine with bromine gives RhSeCl0.5Br0.5 (trigonal, R3m), still Janus, but its chlorine-rich and bromine-rich layers stack so that like faces meet across each gap – selenium against selenium, halogen against halogen. RhSeBr itself also forms, with a lower-symmetry cell that has not yet been refined

How it is made

  • Solid-state reaction 2 Rh + RhCl3 + 3 Se → 3 RhSeCl at 950 °C, which avoids the SeCl4 and Se2Cl2 by-products of the original route from RhCl3 and selenium alone
  • Chemical vapour transport of RhSeCl, including growth with an oscillating temperature profile
  • Self-selecting vapour growth, which gives RhSeCl crystals up to 6 mm across
  • RhTeCl by an adaptation of its first synthesis from 1997, using TeCl4 as the chlorine source
  • Mechanical exfoliation of the crystals to few-layer and monolayer flakes
  • Substituted variants: bromine for chlorine by solid-state reaction and vapour transport; iridium or ruthenium for 20–30% of the rhodium (Rh0.8Ir0.2SeCl, Rh0.7Ru0.3SeCl), so far only with impurity phases

Uses, and how close they are

  • Nonlinear optics and frequency conversion in thin crystalslab
  • Visible-light photodetectorslab

Readiness runs lab → prototype → pilot → deployed.

Open problems

  1. How is charge shared between selenium and chlorine? Structural and magnetic studies describe Rh(III), while X-ray absorption and photoelectron spectra have been read as both anions carrying the same charge
  2. Does a single Janus layer keep the strong second-harmonic response, and how does the response depend on the coupling between layers?
  3. How large is the built-in electric field across one layer, and can it drive spin splitting or photocatalysis in devices?
  4. Its polar symmetry makes RhSeCl piezoelectric and pyroelectric in principle – how large are these responses?

Going deeper

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

For theoreticians · your lens

Calculations give RhSeCl an indirect gap of about 1.2 eV, with the valence-band maximum at Γ and the conduction-band minimum at K, slightly below the optical gap, and attribute its strong second-harmonic response to band nesting. The polar P63mc stacking means interlayer coupling enters the nonlinear susceptibility, and the unusual anion arrangement makes the assignment of charges itself a question worth modelling carefully.

For experimentalists · your lens

Crystals grow by vapour transport and exfoliate with tape. Check phase purity by Raman and composition by EDS, and measure thickness by AFM, because the monolayer Raman spectrum stays close to the bulk. RhSeCl’s missing inversion centre shows directly in second-harmonic generation, a quick test of Janus order. RhTeCl flakes come out needle-shaped, elongated along b, so use polarisation-resolved measurements.

For engineers · your lens

Too new for an engineering assessment: rhodium is expensive, crystals are millimetres across and there is no wafer-scale growth. The device interest is a naturally polar, chemically stable semiconductor for compact nonlinear optics and photodetection.

In the research tracks

Recent news

The newest items tagged RhSeCl, RhTeCl, from the news feed updated 5 Oct 2026.

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Key references

  1. RhTeCl – das erste Chalkogenidhalogenid eines Platinmetalls mit SchichtstrukturKöhler and Urland · Zeitschrift für anorganische und allgemeine Chemie 623, 583 (1997)cited by 11doi:10.1002/zaac.19976230191
  2. Crystal growth of the 2D Janus rhodium chalcohalide RhSeClNowak et al. · Inorganic Chemistry Frontiers 10, 2911 (2023)cited by 13doi:10.1039/D2QI02699F
  3. Exploring the heteroanionic 2D materials RhSeCl and RhTeCl as promising semiconductor materialsNowak et al. · Dalton Transactions 53, 18226 (2024)cited by 4doi:10.1039/D4DT01487A
  4. Synthese, Charakterisierung und Anionenordnung des 2D Janusmaterials RhSeCl und seiner strukturellen AnalogaNowak · Doctoral thesis, TU Dresden (2025)
  5. Optimized synthesis and characterization of Janus RhSeCl with uniform anionic valences, nonlinear optical and optoelectronic propertiesLiu et al. · Advanced Science 12, e05279 (2025)cited by 6doi:10.1002/advs.202505279
  6. Growth of large crystals of Janus phase RhSeCl using self-selecting vapour growthLukovkina et al. · CrystEngComm 28, 1256 (2026)cited by 1doi:10.1039/D5CE01170A
  7. Lattice dynamics of van der Waals layered rhodium chalcochlorides: Janus RhSeCl and 1.5-dimensional RhTeClSchiemenz et al. · Inorganic Chemistry 65, 19169 (2026)doi:10.1021/acs.inorgchem.6c02052