Journal of the American Chemical Society · 2019 · 127 citations · 24 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsCrystal StructureSemiconductor MaterialsCrystal ChemistryCrystal LatticeCrystal SystemsCrystalline MaterialsCrystallographyElectronic Band StructureBand GapCrystal Symmetry DeterminationCrystallographic CharacterizationNonlinear Optical PropertiesOptical Band GapSingle-crystal CrystallographySingle-crystal X-ray DiffractionStructural Determination
Noncentrosymmetric MoS2 semiconductors (1H, 3R) possess not only novel electronic structures of spin–orbit coupling (SOC) and valley polarization but also remarkable nonlinear optical effects. A more interesting noncentrosymmetric structure, the so-called 1T‴-MoS2 layers, was predicted to be built up from [MoS6] octahedral motifs by theoreticians, but the bulk 1T‴ MoS2 or its single crystal structure has not been reported yet. Here, we have successfully harvested 1T‴ MoS2 single crystals by a topochemical method. The new layered structure is determined from single-crystal X-ray diffraction. The crystal crystallizes in space group P31m with a cell of a = b = 5.580(2) Å and c = 5.957(2) Å, which is a √3a × √3a superstructure of 1T MoS2 with corner-sharing Mo3 triangular trimers observed by the STEM. 1T‴ MoS2 is verified to be semiconducting and possesses a band gap of 0.65 eV, different from metallic nature of 1T or 1T′ MoS2. More surprisingly, the 1T‴ MoS2 does show strong optical second-harmonic generation signals. This work provides the first layered noncentrosymmetric semiconductor of edge-sharing MoS6 octahedra for the research of nonlinear optics.
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