of molybdenum disulfide. Scale bar: 1 nm.
Crystalline phases All forms of have a layered structure, in which a plane of molybdenum atoms is sandwiched by planes of sulfide ions. These three strata form a monolayer of . Bulk consists of stacked monolayers, which are held together by weak
van der Waals interactions. Crystalline exists in one of two phases, 2H- and 3R-, where the "H" and the "R" indicate hexagonal and rhombohedral symmetry, respectively. In both of these structures, each molybdenum atom exists at the center of a
trigonal prismatic
coordination sphere and is covalently bonded to six sulfide ions. Each sulfur atom has pyramidal coordination and is bonded to three molybdenum atoms. Both the 2H- and 3R-phases are semiconducting. A third, metastable crystalline phase known as 1T- was discovered by intercalating 2H- with
alkali metals. This phase has trigonal symmetry and is metallic. The 1T-phase can be stabilized through doping with electron donors such as
rhenium, or converted back to the 2H-phase by microwave radiation. The 2H/1T-phase transition can be controlled via the incorporation of sulfur (S)
vacancies.
Allotropes Nanotube-like and
buckyball-like molecules composed of are known.
Exfoliated flakes While bulk in the 2H-phase is known to be an indirect-band gap semiconductor, monolayer has a direct band gap. The layer-dependent optoelectronic properties of have promoted much research in 2-dimensional -based devices. 2D can be produced by exfoliating bulk crystals to produce single-layer to few-layer flakes either through a dry, micromechanical process or through solution processing. Micromechanical exfoliation, also pragmatically called "
Scotch-tape exfoliation", involves using an adhesive material to repeatedly peel apart a layered crystal by overcoming the van der Waals forces. The crystal flakes can then be transferred from the adhesive film to a substrate. This facile method was first used by
Konstantin Novoselov and
Andre Geim to obtain graphene from graphite crystals. However, it can not be employed for a uniform 1-D layers because of weaker adhesion of to the substrate (either silicon, glass or quartz); the aforementioned scheme is good for graphene only. While Scotch tape is generally used as the adhesive tape,
PDMS stamps can also satisfactorily cleave if it is important to avoid contaminating the flakes with residual adhesive. Liquid-phase exfoliation can also be used to produce monolayer to multi-layer in solution. A few methods include lithium
intercalation to delaminate the layers and
sonication in a high-surface tension solvent.
Mechanical properties excels as a lubricating material (see below) due to its layered structure and low
coefficient of friction. Interlayer sliding dissipates energy when a shear stress is applied to the material. Extensive work has been performed to characterize the coefficient of friction and shear strength of in various atmospheres. The
shear strength of increases as the coefficient of friction increases. This property is called
superlubricity. At ambient conditions, the coefficient of friction for was determined to be 0.150, with a corresponding estimated shear strength of 56.0 MPa. The wear resistance of in lubricating applications can be increased by
doping with
Cr. Microindentation experiments on
nanopillars of Cr-doped found that the yield strength increased from an average of 821 MPa for pure (at 0% Cr) to 1017 MPa at 50% Cr. The increase in yield strength is accompanied by a change in the failure mode of the material. While the pure nanopillar fails through a plastic bending mechanism, brittle fracture modes become apparent as the material is loaded with increasing amounts of dopant. In recent years, has been utilized in flexible electronic applications, promoting more investigation into the elastic properties of this material. Nanoscopic bending tests using
AFM cantilever tips were performed on micromechanically exfoliated flakes that were deposited on a holey substrate. The Young's modulus of monolayer flakes was 270 GPa, Bertolazzi and coworkers also characterized the failure modes of the suspended monolayer flakes. The strain at failure ranges from 6 to 11%. The average yield strength of monolayer is 23 GPa, which is close to the theoretical fracture strength for defect-free . == Chemical reactions ==