Tantalum disulfide and diselenide

TaS₂, TaSe₂, TaTe₂

Also called TaS₂, 1T-TaS₂, 2H-TaS₂, TaSe₂

van der Waals crystal depends on form

A material with a rich menu of electronic states. As it cools, 1T-TaS2 passes through several phases in which electrons clump into star-shaped clusters, ending as an insulator; a short laser or voltage pulse can flip it into a hidden metallic state that persists. That switchable memory makes it interesting for ultrafast electronics, and its ground state is a candidate quantum spin liquid. TaSe2 forms the same charge-density-wave patterns but stays metallic, which helps separate what the lattice distortion does from what electron correlations do.

Crystal structure

  • Ta
  • S
Cell
Hexagonal, a = 3.36 Å
Atoms per cell
3
Ta–S bond
2.44 Å
Height
2.95 Å between the outer atom centres
In the 1T structure the lower sulfur plane is turned against the upper one, so each tantalum atom sits in an octahedron rather than a prism, and the layer has an inversion centre. On cooling, the Ta atoms pull together into 13-atom ‘Star of David’ clusters, which lock into a commensurate √13×√13 superlattice below about 180 K. The model shows the undistorted lattice the stars form from. Average 1T cell: a = 3.36 Å, c = 5.90 Å, with sulfur at the ideal height of the CdI2 structure type, a quarter of c above and below the Ta plane.

Key properties

  • Sequence of charge-density-wave phases in bulk 1T-TaS2: incommensurate below ~550 K, nearly commensurate below ~350 K, commensurate below ~180 K on cooling
  • A single femtosecond laser pulse, or a short voltage pulse, switches it into a metastable hidden metallic state
  • Gate-controlled phase transitions in thin flakes, including suppression of the charge density wave and emergence of superconductivity
  • Triangular lattice of Star-of-David clusters with one unpaired electron each – a proposed quantum spin liquid
  • 2H-TaS2 superconductivity strengthens in thin flakes, from ~0.8 K in bulk to a few kelvin in the monolayer
  • 2H-TaSe2: incommensurate charge density wave below ~122 K, locking into a commensurate one at ~90 K
  • 1T-TaSe2: commensurate √13×√13 charge density wave below ~473 K, yet metallic in bulk

How it is made

  • Vapour-transport growth with iodine – quenching from high temperature retains 1T, slow cooling gives 2H
  • Mechanical exfoliation, with encapsulation for transport work
  • CVD growth of thin crystals

Uses, and how close they are

  • Ultrafast memristive switches and oscillatorslab
  • Model system for Mott and spin-liquid physicslab

Readiness runs lab → prototype → pilot → deployed.

Open problems

  1. Is bulk 1T-TaS2 a Mott insulator, or a band insulator created by pairing of layers along the stacking direction?
  2. What is the hidden metallic state, and can it be written and erased reliably in devices at practical temperatures?
  3. Is there a quantum spin liquid in 1T-TaS2 or in related 1T-TaSe2 monolayers?

Going deeper

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

For theoreticians · your lens

Correlations and stacking compete: DFT+U or DMFT on a single Star-of-David layer gives a Mott insulator, but interlayer dimerisation in bulk can open a gap without correlations. Faithful models need the 13-atom charge-density-wave supercell, the stacking sequence and spin–orbit coupling.

For experimentalists · your lens

Resistivity hysteresis between ~180 K on cooling and ~220 K on warming is the fingerprint of the commensurate transition in bulk; it shifts and broadens in thin flakes. STM images the Star-of-David pattern directly, and ultrafast pump–probe and ARPES follow the charge-density-wave dynamics.

For engineers · your lens

Offers non-volatile resistive switching on picosecond timescales, but many useful phases sit below room temperature and device reproducibility is unproven.

In the research tracks

Recent news

The newest items tagged TaS2, TaSe2, from the news feed updated 5 Oct 2026.

Preprintnot yet peer reviewed arXiv

Equilibrium Stabilization of a Hidden Phase Like Metallic State in 1T-TaS2

Electronic phases that lie outside the equilibrium ground state offer a route to explore competing configurations in correlated materials. In 1T-TaS2, ultrafast excitation accesses a metallic hidden phase that is distinct from the commensurate insulating ground state. Here we use angle-resolved photoemission…

ExperimentTaS₂, TaSe₂
Journal Nano Letters

Discovery and Manipulation of a Single Polaron in a Monolayer Mott Insulator

Polarons are quasiparticles composed of excess electrons and local lattice distortions that are crucial for understanding many-body physics. However, atomic-scale observation and manipulation of an intrinsic polaron in strongly correlated systems still remain elusive. Here, we report the discovery and manipulation of a…

ExperimentTheoryTaS₂, TaSe₂
Preprintnot yet peer reviewed arXiv

Moiré Mott correlated mosaics in twisted bilayer 1T-TaS2

The tunability and twist engineering of van der Waals materials enable the emergence of electronic states not present in individual monolayers. Among them, monolayer 1T-TaS2 is a well-known Mott insulating system, whose star-of-David charge density wave reconstruction realizes an emergent triangular lattice of local…

All 17 items tagged TaS₂, TaSe₂ in the news feed  ·  RSS feed for TaS₂, TaSe₂

Key references

  1. Ultrafast switching to a stable hidden quantum state in an electronic crystalStojchevska et al. · Science 344, 177 (2014)cited by 725doi:10.1126/science.1241591
  2. Gate-tunable phase transitions in thin flakes of 1T-TaS2Yu et al. · Nature Nanotechnology 10, 270 (2015)cited by 760doi:10.1038/nnano.2014.323
  3. Charge-density waves and superlattices in the metallic layered transition metal dichalcogenidesWilson, DiSalvo and Mahajan · Advances in Physics 24, 117 (1975)cited by 2,237doi:10.1080/00018737500101391