2017
DOI: 10.1016/j.jallcom.2016.12.433
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Characters of group V and VII atoms doped WSe 2 monolayer

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Cited by 15 publications
(4 citation statements)
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“…The energy bands of I-doped MoTe 2 systems are highly dense and show a significant shift to the lower energy area. Subsequently, impurity levels cross the Fermi level, making all doped systems exhibit metallic behavior, which is a typical characteristic of n-type doping. , In addition, with the increase in the I concentration, the bandwidth of I-doped MoTe 2 systems decreases due to the increase in the impurity level close to the Fermi level. As a result, each donor impurity removes a state from the conduction band and establishes it as an impurity level of lower energy in the interband.…”
Section: Resultsmentioning
confidence: 99%
“…The energy bands of I-doped MoTe 2 systems are highly dense and show a significant shift to the lower energy area. Subsequently, impurity levels cross the Fermi level, making all doped systems exhibit metallic behavior, which is a typical characteristic of n-type doping. , In addition, with the increase in the I concentration, the bandwidth of I-doped MoTe 2 systems decreases due to the increase in the impurity level close to the Fermi level. As a result, each donor impurity removes a state from the conduction band and establishes it as an impurity level of lower energy in the interband.…”
Section: Resultsmentioning
confidence: 99%
“…To evaluate the thermodynamical stability of the doped materials, the formation energy is calculated according to the equation Enormalf=EdopedEpure+mnmμm$$\begin{eqnarray}{E}_{\mathrm{f}} = {E}_{{\mathrm{doped}}} - {E}_{{\mathrm{pure}}} + \sum_m {{n}_m} {\mu }_m\end{eqnarray}$$where E doped and E pure are the total energies of the supercells with and without doped atoms, respectively; n m is the number of m atom added ( n m < 0) or removed ( n m > 0); µ m is the chemical potential of the bulk element m , which is the energy of per atom obtained from the corresponding bulk material. [ 35–37 ]…”
Section: Theoriesmentioning
confidence: 99%
“…where E doped and E pure are the total energies of the supercells with and without doped atoms, respectively; n m is the number of m atom added (n m < 0) or removed (n m > 0); μ m is the chemical potential of the bulk element m, which is the energy of per atom obtained from the corresponding bulk material. [35][36][37] The plasma frequency and the dynamic dielectric function can be obtained from Vienna Ab initio Simulation Package (VASP) directly, whose imaginary part yields the absorption spectra. Generally, the absorbance of 2D materials is given by [38] A…”
Section: Theoriesmentioning
confidence: 99%
“…Recently, it has been reported that most TMDs adsorb gas as physical adsorption and the effect is not ideal. Therefore, it is essential to enhance the effect of adsorption gas through different means, for example, by doping, vacancies, and other forms of intrinsic material modification to improve the adsorption of harmful gases. Zhao et al improved the gas molecule adsorption by doping Cu atoms on MoS 2 ; Cui et al studied the effect of Pt atom-doped HfSe 2 monolayers on the adsorption properties of SO 2 and SOF 2 molecules; and Liu et al studied the adsorption characteristics of the TM (Ag, Pd, Pt, Rh, and Ru)-modified WSe 2 for a SF 6 decomposition gas . The influence of a single vacancy and Si-doped GeS on the sensitivity of SF 6 and other gases has been studied by Gao et al…”
Section: Introductionmentioning
confidence: 99%