Spin–orbit coupling tunable electronic properties of [formula omitted]-MoS[formula omitted] and ternary Janus [formula omitted]-MoSSe monolayers: Theoretical prediction

Abstract

MoS2 can exist in many different polytypes, such as trigonal prismatic, distorted octahedral, or octahedral. The 2H-phase of MoS2 has been extensively studied in recent times, but there are very few studies focusing on the remaining phases, especially the distorted octahedral T′)-phase. Here, we design the MoS2 monolayer and Janus MoSSe structure in the 1T′ phase and study their electronic properties within the framework of first-principles calculations. Both 1T′-MoS2 and 1T′-MoSSe monolayers are confirmed to have structural stability and anisotropic mechanical characteristics. Interestingly, while the 1T′-MoS2 monolayer exhibits metallic characteristics, Janus MoSSe in the 1T′ phase is a semiconductor with a small band gap of 0.04 eV. More interestingly, a tiny bandgap of 0.05 eV has opened up in the 1T′-MoS2 monolayer due to the spin–orbit coupling effect. We also study the mobility of carriers in the semiconductor Janus 1T′-MoSSe monolayer. 1T′-MoSSe monolayer exhibits a high anisotropic carrier mobility due to its high anisotropic crystal structure. Surprisingly, 1T′-MoSSe monolayer possesses extremely high electron mobility, up to 4.58×103 cm2 V−1 s−1. Our findings give a deeper insight into the 1T′-phase of transition metal dichalcogenide and its Janus structure.