Tunable inverted gap detected in quasi-metallic molybdenum disulfide monolayer
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Tunable inverted gap detected in quasi-metallic molybdenum disulfide monolayer
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research team led by Andrew T.S. Wee and Andrivo Rusydi from the National University of Singapore has experimentally observed a tunable inverted gap (~0.5 eV) and a fundamental gap (~0.1 eV) in quasi-metallic monolayer molybdenum disulfide (MoS2). By providing insight into the origins of the inverted gap and the phase transition of the monolayer (MoS2) on a gold film, this work offers enhanced fundamental understanding of two-dimensional-transitionmetal dichalcogenides (2D-TMDs). This study was carried out in collaboration with researchers at Shenzhen University in China and was recently published in Nature Communications (doi:10.1038/ s41467-017-00640-2). Xinmao Yin, a visiting research fellow and the main author of this study, says that by providing a deeper understanding of the intrinsic properties of polymorphic
MoS2, their results unlock bigger possibilities for 2D-TMD-based optoelectronic device applications. Two-dimensional MoS 2 exhibits polymorphism, with a trigonal semiconducting 1H phase transition to an octahedral metallic 1T phase, which then spontaneously relaxes to a distorted quasi-metallic 1T ʹ phase. The research group designed a new annealing-based strategy to induce a semiconductorto-metal phase transition in monolayer MoS2 on gold in order to study the metastable 1T ʹ monolayer MoS 2 phase. The samples were annealed at different temperatures in vacuum and the temperature window of 200–250°C was found to be the optimal condition for the 1H-1Tʹ phase transition. The phase transition has been attributed to electron transfer from the gold to the MoS2, where this is further facilitated by interfacial strain. Previously, a theoretical study published in Science (doi:10.1126/science.1256815) predicted that spin–orbit coupling might open up a fundamental
The different crystal structures of monolayer MoS2 and the observed tunable inverted gap and fundamental gap. Image provided by Xinmao Yin, Wenjing Zhang, Andrivo Rusydi, and Andrew T.S. Wee.
gap (~0.1 eV) in the distorted octahedral structure (1Tʹ phase) of 2D-TMDs. This theoretical work also predicted a larger inverted gap (~0.6 eV) in the 1Tʹ structure. The nondestructive technique of spectroscopic ellipsometry was used to detect the optical gaps. The mid-infrared peak observed at ~0.5 eV was assigned to the 1Tʹ-MoS2 inverted gap, which could be tuned via the interfacial strain. This was attributed to a coupling of a distorted lattice and electron–electron correlations, which demonstrated the presence of strong charge-lattice coupling in 1Tʹ 2D-TMDs. A far-infrared peak was observed at ~0.10 eV. This corresponded to the fundamental gap and arises due to strong spin–orbit coupling. Changes in optical and electronic properties were also monitored in a comprehensive research study involving transport, Raman, photoluminescence, and synchrotron-based photoemission spectroscopy (PES), and showed that the transition from the 1H to the 1Tʹ phase is optimized by annealing the
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