Titanium, zirconium and hafnium dichalcogenides

MX₂ (M = Ti, Zr, Hf; X = S, Se, Te)

Also called TiS₂, TiSe₂, TiTe₂, ZrS₂, ZrSe₂, ZrTe₂, HfS₂, HfSe₂

van der Waals crystal depends on form

The titanium, zirconium and hafnium compounds share one simple layer structure but range from battery material to exotic electronic states. TiS2 was the cathode of the first rechargeable lithium battery in the 1970s. TiSe2 turns into a charge-density wave near 200 K, and may be one of the rare crystals in which electrons and holes pair up into a condensate of excitons. HfSe2 and ZrSe2 are semiconductors whose surfaces oxidise into hafnium and zirconium oxide – the high-κ insulators the chip industry already relies on – so they can grow their own gate dielectric.

Crystal structure

  • Ti
  • Se
Cell
Hexagonal, a = 3.54 Å
Atoms per cell
3
Ti–Se bond
2.54 Å
Height
3.00 Å between the outer atom centres
Titanium between two selenium planes that are turned against each other, so each Ti atom sits in an octahedron: the 1T structure shared by the titanium, zirconium and hafnium dichalcogenides. Below about 200 K the atoms of TiSe2 shift slightly into a 2×2×2 superlattice; the model shows the undistorted layer. Bulk 1T-TiSe2: a = 3.54 Å, c = 6.01 Å, with selenium placed at the ideal height of the CdI2 structure type, a quarter of c above and below the Ti plane.

Key properties

  • TiSe2: a 2×2×2 charge-density wave below ~200 K; electron–hole (excitonic) pairing is a leading explanation, and signatures of exciton condensation were reported in 2017
  • Copper intercalation or electrostatic gating suppresses the charge-density wave in TiSe2 and makes it superconducting at a few kelvin
  • Single-layer TiTe2 develops a 2×2 charge-density wave below ~92 K that is absent in thicker layers
  • HfSe2 and ZrSe2: gaps of 0.9–1.2 eV and oxidation into high-κ HfO2 or ZrO2; few-layer transistors reach on/off ratios above 106
  • Stoichiometric TiS2 is a semiconductor with a ~0.5 eV indirect gap, but excess titanium makes most crystals conduct like metals
  • ZrTe2 is a Dirac semimetal down to a single layer and has been used as a low-resistance contact for MoS2 transistors

How it is made

  • Chemical vapour transport with iodine for bulk crystals
  • Molecular beam epitaxy of single layers, such as TiSe2 and TiTe2 on bilayer graphene and ZrTe2 on InAs
  • Mechanical exfoliation, and controlled oxidation of HfSe2 and ZrSe2 to form their native oxides
  • Intercalation of lithium, copper and other ions between the layers

Uses, and how close they are

  • Lithium and sodium battery electrodes (TiS2)prototype
  • Transistors that grow their own high-κ gate dielectric (HfSe2, ZrSe2)lab
  • Low-resistance semimetal contacts for 2D transistors (ZrTe2)lab

Readiness runs lab → prototype → pilot → deployed.

Open problems

  1. Is the charge-density wave in TiSe2 driven by exciton condensation, by electron–phonon coupling, or by both working together?
  2. Why does a charge-density wave appear in single-layer TiTe2 but not in thicker flakes?
  3. Can native HfO2 or ZrO2 grown on HfSe2 and ZrSe2 approach the interface quality of silicon with its oxide?

Going deeper

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

For theoreticians · your lens

With a formally d0 metal, these compounds test band-gap physics directly: the small indirect gaps between chalcogen p and metal d states are badly underestimated by semilocal DFT, and whether TiS2 or TiSe2 comes out as a semimetal depends on the method, so GW and careful defect calculations are needed. TiSe2 adds the excitonic-insulator question – its charge-density wave can be driven by electron–hole attraction or by a Jahn–Teller-like lattice instability, and realistic models include both.

For experimentalists · your lens

Composition matters: excess titanium dopes TiS2 and TiSe2 strongly, so report stoichiometry and growth temperature. The TiSe2 transition appears as a resistivity anomaly near 200 K and as folded bands in ARPES; momentum-resolved EELS and ultrafast probes test the excitonic picture. For HfSe2 and ZrSe2, follow oxidation with Raman and XPS.

For engineers · your lens

HfSe2 and ZrSe2 are the members to watch for chips: a semiconductor with a gap close to silicon’s that can form its own high-κ dielectric addresses one of the hardest integration steps for 2D transistors, although wafer-scale growth and oxide interface quality remain open. TiS2 has a long battery history but was displaced by oxide cathodes.

In the research tracks

Recent news

The newest items tagged TiSe2, ZrSe2, HfSe2, from the news feed updated 5 Oct 2026.

Journal Nanotechnology (IOP)

Exfoliation-induced increase in van der Waals gap in two-dimensional layered crystals

This work demonstrates that mechanical exfoliation induces measurable distortions in the van der Waals (vdW) gap of layered crystals, while the annealing process can reduce this distortion. Using x-ray diffraction, lattice parameters were compared in bulk and mechanically exfoliated flakes of selected transition metal…

Preprintnot yet peer reviewed arXiv

Crystallographic and Electronic Phase Changes in TiTe2 via Atmospheric and Electron Beam Exposure

In this study, we examine the surface sensitivity of a transition metal dichalcogenide (TiTe2) grown using the Chemical Vapor Transport (CVT) technique at high pressure and study the surface changes in the sample upon exposure to air as well as its crystallographic properties upon e-beam exposure. We examine the local…

Preprintnot yet peer reviewed arXiv

Interplay of Excitonic Charge Density Wave and Superconductivity in Transition Metal Dichalcogenides

Motivated by the unique characteristics of the phase diagram of 1T-TiSe2, we investigated the complex interplay of excitonic charge density wave (CDW) and superconductivity (SC) on a two-dimensional triangular lattice, each site accommodating two orbitals. In response to various tuning parameters, such as…

All 17 items tagged TiSe₂, ZrSe₂, HfSe₂ in the news feed  ·  RSS feed for TiSe₂, ZrSe₂, HfSe₂

Key references

  1. Electrical energy storage and intercalation chemistryWhittingham · Science 192, 1126 (1976)cited by 1,927doi:10.1126/science.192.4244.1126
  2. Electronic properties and superlattice formation in the semimetal TiSe2Di Salvo et al. · Physical Review B 14, 4321 (1976)cited by 645doi:10.1103/PhysRevB.14.4321
  3. Superconductivity in CuxTiSe2Morosan et al. · Nature Physics 2, 544 (2006)cited by 997doi:10.1038/nphys360
  4. Signatures of exciton condensation in a transition metal dichalcogenideKogar et al. · Science 358, 1314 (2017)cited by 482doi:10.1126/science.aam6432
  5. HfSe2 and ZrSe2: two-dimensional semiconductors with native high-κ oxidesMleczko et al. · Science Advances 3, e1700481 (2017)cited by 297doi:10.1126/sciadv.1700481
  6. Emergence of charge density waves and a pseudogap in single-layer TiTe2Chen et al. · Nature Communications 8, 516 (2017)cited by 131doi:10.1038/s41467-017-00641-1
  7. Massless Dirac fermions in ZrTe2 semimetal grown on InAs(111) by van der Waals epitaxyTsipas et al. · ACS Nano 12, 1696 (2018)cited by 103doi:10.1021/acsnano.7b08350