Molybdenum ditelluride

MoTe₂

Also called 2H-MoTe₂, 1T′-MoTe₂, Td-MoTe₂

van der Waals crystal depends on form

Molybdenum ditelluride can be a semiconductor or a metal depending on how its atoms are arranged, and the energy difference between the two arrangements is small enough to switch with heat, strain or a laser – so metal contacts and semiconductor channels can be patterned into the same sheet. Twisted bilayers of the semiconducting form produced the first fractional quantum anomalous Hall effect, in 2023.

Crystal structure

  • Mo
  • Te
Cell
Hexagonal, a = 3.52 Å
Atoms per cell
3
Mo–Te bond
2.68 Å
Height
3.49 Å between the outer atom centres
The same trigonal-prismatic sandwich as MoS2, with tellurium in place of sulfur: the larger atoms stretch the lattice to 3.52 Å and make the layer 3.5 Å thick from tellurium to tellurium. MoTe2 is the member of the family whose octahedral 1T′ form is almost as stable as this one, which is why the two can be switched with strain, gating or a laser. The model shows the semiconducting phase. One layer of bulk 2H-MoTe2 (Puotinen and Newnham, Acta Crystallographica 14, 691, 1961; COD 2310465): a = 3.52 Å, tellurium planes 1.75 Å above and below the Mo plane.

Key properties

  • Small 2H–1T′ energy difference (tens of meV per formula unit) allows phase switching by heating, strain, gating or laser irradiation
  • 2H monolayer optical gap ~1.1 eV – a near-infrared emitter matched to silicon photonics wavelengths
  • Td-MoTe2 is a candidate type-II Weyl semimetal; bulk superconductivity below ~0.1 K rises to several kelvin under pressure
  • Fractional quantum anomalous Hall effect in twisted bilayer 2H-MoTe2 at twist angles near 3.5–4° (2023)

How it is made

  • Vapour-transport or flux growth of bulk crystals; quenching favours 1T′, slow cooling favours 2H
  • CVD or tellurisation of Mo films, with the phase selected by tellurium supply and temperature
  • Laser-induced 2H → 1T′ conversion to write metallic contacts into semiconducting flakes

Uses, and how close they are

  • Phase-engineered ohmic contacts for 2D transistorslab
  • Near-infrared emitters and detectors compatible with silicon photonicslab
  • Topological and fractional quantum Hall physics (twisted MoTe2)lab

Readiness runs lab → prototype → pilot → deployed.

Open problems

  1. Can 2H/1T′ phase patterning be made reproducible and stable enough for a lateral-contact technology?
  2. What decides the competition between fractional Chern insulators, charge order and superconductivity in twisted MoTe2?
  3. Does the topological character of Td-MoTe2 survive in few-layer samples?

Going deeper

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

For theoreticians · your lens

Near-degenerate polymorphs make total energies sensitive to functional, dispersion correction and spin–orbit coupling – check phase rankings with several methods before trusting them. In twisted 2H-MoTe2 the topmost moiré valence bands carry nonzero Chern numbers with layer-pseudospin skyrmion textures, and exact diagonalisation of projected continuum models reproduces the fractional states.

For experimentalists · your lens

Distinguish phases by Raman: 2H shows A1g near 171 cm−1 and E12g near 234 cm−1; 1T′ shows modes near 127, 161 and 256 cm−1, and the 1T′–Td transition around 250 K appears in low-frequency shear modes. Work in a glovebox.

For engineers · your lens

Attractive as a way to make contacts and channels from one material, with a band gap suited to silicon photonics, but air sensitivity and phase instability are serious obstacles to manufacturing.

In the research tracks

Recent news

The newest items tagged MoTe2, from the news feed updated 5 Oct 2026.

Preprintnot yet peer reviewed arXiv

Parafermions in fractional Chern insulator-superconductor heterostructures: the role of spin polarization

Most proposals for Z3 parafermions in fractional quantum Hall-superconductor structures used the spin-unpolarized ν= 2/3 Halperin (1,1,2) state. The fractional quantum anomalous Hall (FQAH) states of twisted MoTe2 and rhombohedral graphene are believed to be spin- and valley-polarized Jain states, with the same…

Preprintnot yet peer reviewed arXiv

Ferroelectric Hysteresis in Superconducting Bilayer Td-MoTe2

Recently, the displacement-field-driven hysteretic switching of superconductivity was reported in ferroelectric bilayer Td-MoTe2. Such direct coupling between ferroelectricity and superconductivity offers promising pathways for low-power, non-volatile memory devices, but the underlying coupling mechanism remains poorly…

TheoryMoTe₂
Preprintnot yet peer reviewed arXiv

First-Principles Study of I2 and CH3I Adsorption on Transition Metal Decorated 2D-Material substrates : Insights from Electronic Structure and Reaction Kinetics

Radioactive iodine species, particularly I2 and CH3I, pose significant environmental and technological hazards owing to their high volatility, chemical stability, and relatively weak interaction with traditional substrate and sorption materials. In this work, we proposed a series of transition-metal (TM) (Fe, Ni, Cu…

Preprintnot yet peer reviewed arXiv

Interlayer Fermi Polarons in Bilayer MoTe2

Atomic bilayers of transition metal dichalcogenides (TMDs) host quantum phases governed by the layer degree of freedom, including bilayer Wigner crystals, fractional Chern insulators, and exciton condensates. These phases are probed primarily through exciton spectroscopy, yet it remains poorly understood how excitons…

TheoryMoTe₂
Preprintnot yet peer reviewed arXiv

Zoology of chiral superconductors in Chern bands

Evidence for chiral superconductivity has recently been observed in several van der Waals systems including rhombohedral multilayer graphene and twisted bilayer MoTe2. In the latter, superconductivity emerges at carrier densities near a fractional Chern insulator. This raises the question of what kinds of…

All 30 items tagged MoTe₂ in the news feed  ·  RSS feed for MoTe₂

Key references

  1. Phase patterning for ohmic homojunction contact in MoTe2Cho et al. · Science 349, 625 (2015)cited by 1,182doi:10.1126/science.aab3175
  2. Bandgap opening in few-layered monoclinic MoTe2Keum et al. · Nature Physics 11, 482 (2015)cited by 1,034doi:10.1038/nphys3314
  3. Signatures of fractional quantum anomalous Hall states in twisted MoTe2Cai et al. · Nature 622, 63 (2023)cited by 718doi:10.1038/s41586-023-06289-w