Tungsten diselenide is an inorganic compound with the formula WSe<sub>2</sub>. The compound adopts a hexagonal crystalline structure similar to molybdenum disulfide. The tungsten atoms are covalently bonded to six selenium ligands in a trigonal prismatic coordination sphere while each selenium is bonded to three tungsten atoms in a pyramidal geometry. The tungstenâÂÂselenium bond has a length of 0.2526 nm, and the distance between selenium atoms is 0.334 nm. It is a well studied example of a layered material. The layers stack together via van der Waals interactions. WSe<sub>2</sub> is a very stable semiconductor in the group-VI transition metal dichalcogenides.
The hexagonal (P6<sub>3</sub>/mmc) polymorph 2H-WSe<sub>2</sub> is isotypic with hexagonal MoS<sub>2</sub>. The two-dimensional lattice structure has W and Se arranged periodically in layers with hexagonal symmetry. Similar to graphite, van der Waals interactions hold the layers together; however, the 2D-layers in WSe<sub>2</sub> are not atomically thin. The large size of the W cation renders the lattice structure of WSe<sub>2</sub> more sensitive to changes than MoS<sub>2</sub>.
In addition to the typical semiconducting hexagonal structure, a second metallic polymorph of WSe<sub>2</sub> exists. This phase, 1T-WSe<sub>2</sub>, is based on a tetragonal symmetry with one WSe<sub>2</sub> layer per repeating unit. The 1T-WSe<sub>2</sub> phase is less stable and transitions to the 2H-WSe<sub>2</sub> phase. WSe<sub>2</sub> can form a fullerene-like structure.
The Young's modulus varies greatly as a function of the number of layers in a flake. For a single monolayer, the reported Young's modulus is 258.6 ñ 38.3 GPa.
Heating thin films of tungsten under pressure from gaseous selenium and high temperatures (>800 K) using the sputter deposition technique leads to the films crystallizing in hexagonal structures with the correct stoichiometric ratio.
The potential applications of transition metal dichalcogenides in solar cells and photonics are often discussed. Bulk has an optical band gap of ~1.35 eV with a temperature dependence of âÂÂ4.6 eV/K. photoelectrodes are stable in both acidic and basic conditions, making them potentially useful in electrochemical solar cells.
The properties of monolayers differ from those of the bulk state, as is typical for semiconductors. Mechanically exfoliated monolayers of are transparent photovoltaic materials with LED properties. The resulting solar cells pass 95 percent of the incident light, with one tenth of the remaining five percent converted into electrical power. The material can be changed from p-type to n-type by changing the voltage of an adjacent metal electrode from positive to negative, allowing devices made from it to have tunable bandgaps.
Superconductivity has been reported in twisted bilayer , with a transition temperature of 200 mK.