Abstract

Based on the density functional theory (DFT), the electronic properties of O-doped pure and sulfur vacancy-defect monolayer WS2 are investigated by using the first-principles method. For the O-doped pure monolayer WS2, four sizes (2 × 2 × 1, 3 × 3 × 1, 4 × 4 × 1 and 5 × 5 × 1) of supercell are discussed to probe the effects of O doping concentration on the electronic structure. For the 2 × 2 × 1 supercell with 12.5% O doping concentration, the band gap of O-doped pure WS2 is reduced by 8.9% displaying an indirect band gap. The band gaps in 3 × 3 × 1 and 4 × 4 × 1 supercells are both opened to some extent, respectively, for 5.55% and 3.13% O doping concentrations, while the band gap in 5 × 5 × 1 supercell with 2.0% O doping concentration is quite close to that of the pure monolayer WS2. Then, two typical point defects, including sulfur single-vacancy (VS) and sulfur divacancy (V2S), are introduced to probe the influences of O doping on the electronic properties of WS2 monolayers. The observations from DFT calculations show that O doping can broaden the band gap of monolayer WS2 with VS defect to a certain degree, but weaken the band gap of monolayer WS2 with V2S defect. Doping O element into either pure or sulfur vacancy-defect monolayer WS2 cannot change their band gaps significantly, however, it still can be regarded as a potential method to slightly tune the electronic properties of monolayer WS2.

Highlights

  • Two-dimensional (2D) transition-metal dichalcogenides (TMD), such as MoS2, WS2 and others, have been widely studied because of their excellent properties in mechanics, electronics, optics and so on

  • We focus on the influences of oxygen (O) element on the electronic properties of both pure monolayer WS2 and two types of sulfur vacancy-defects monolayer WS2, including S

  • The electronic properties of O-doped pure and sulfur vacancy-defect WS2 monolayers are studied using first-principles calculations based on the density functional theory (DFT)

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Summary

A First-Principles Study

Department of Mechanical Engineering, Northwestern University, eVanston, IL 60208, USA School of Mechanical Engineering and Automation, Fuzhou University, Fuzhou 350108, China Received: 23 November 2017; Accepted: 29 January 2018; Published: 31 January 2018

Introduction
Physical Modeling and Simulation Methods
Structure Properties
The bond length of the
O-Doped Pure WS2
O-Doped Sulfur Vacancy-Defect WS2
The band gap size of aofWS
Compared with band in Table
Conclusions

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