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Tungsten diselenide

Tungsten diselenide
STM of WSe2 on HOPG.jpg
WSe2 monolayer on graphite (yellow) and its atomic image (inset)
Molybdenite-3D-balls.png
Identifiers
3D model (JSmol)
ECHA InfoCard 100.031.877
EC Number 235-078-7
PubChem CID
Properties
WSe2
Molar mass 341.76 g/mol
Appearance grey to black solid
Odor odorless
Density 9.32 g/cm3
Melting point > 1200 °C
insoluble
Band gap ~1 eV (indirect, bulk)
~1.7 eV (direct, monolayer)
Structure
hP6, space group P6
3
/mmc, No 194
a = 0.3297 nm, c = 1.2982 nm
Trigonal prismatic (WIV)
Pyramidal (Se2−)
Hazards
Main hazards External MSDS
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa).
Infobox references

Tungsten diselenide is an inorganic compound with the formula WSe2. The compound adopts a hexagonal crystalline structure similar to molybdenum disulfide. Every tungsten atom is 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 tungsten–selenium bond has a length of 0.2526 nm, and the distance between selenium atoms is 0.334 nm. Layers stack together via van der Waals interactions. WSe2 is a very stable semiconductor in the group-VI transition metal dichalcogenides.

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.

Transition metal dichalcogenides are semiconductors with potential applications in solar cells. WSe
2
has a band-gap of ~1.35 eV with a temperature dependence of −4.6×104 eV/K.WSe
2
photoelectrodes are stable in both acidic and basic conditions, making them potentially useful in electrochemical solar cells.

The properties of WSe
2
monolayers differ from those of the bulk state, as is typical for semiconductors. Mechanically exfoliated monolayers of WSe
2
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. As a result, it may enable LEDs of any color to be made from a single material.


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