2019
DOI: 10.1016/j.apsusc.2019.02.218
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Temperature controlled 1T/2H phase ratio modulation in mono- and a few layered MoS2 films

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Cited by 35 publications
(18 citation statements)
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“…When the pressure is low (e.g., 0.8 Pa), the number of crystal nuclei per unit volume is large, and the bonding between crystal grains is not dense, resulting in high surface roughness. As the pressure increases, voids are reduced to increase the compactness and uniformity of the films, to smooth the surfaces, and lower the roughness [40]. The To investigate the grain growth and crystal structure of the MoS 2 films, we analyzed the peak half width of the (202) plane of MoS 2 on the basis of Bragg's equation (Equation 1), the cubic system distance in Equation 2, and Scherrer's equation (Equation 3), which can be used to calculate the interplanar spacing (d), lattice constant (a), and average grain size (D) [35], respectively:…”
Section: Resultsmentioning
confidence: 99%
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“…When the pressure is low (e.g., 0.8 Pa), the number of crystal nuclei per unit volume is large, and the bonding between crystal grains is not dense, resulting in high surface roughness. As the pressure increases, voids are reduced to increase the compactness and uniformity of the films, to smooth the surfaces, and lower the roughness [40]. The To investigate the grain growth and crystal structure of the MoS 2 films, we analyzed the peak half width of the (202) plane of MoS 2 on the basis of Bragg's equation (Equation 1), the cubic system distance in Equation 2, and Scherrer's equation (Equation 3), which can be used to calculate the interplanar spacing (d), lattice constant (a), and average grain size (D) [35], respectively:…”
Section: Resultsmentioning
confidence: 99%
“…When the pressure is low (e.g., 0.8 Pa), the number of crystal nuclei per unit volume is large, and the bonding between crystal grains is not dense, resulting in high surface roughness. As the pressure increases, voids are reduced to increase the compactness and uniformity of the films, to smooth the surfaces, and lower the roughness [40]. The surface morphology of the MoS 2 films directly affects the diffuse scattering, absorption, and transmission of incident light, which are key to their different optical band gaps.…”
Section: Resultsmentioning
confidence: 99%
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“…Using Scherrer's formula, the grain size in 1 T and 2H phases is 6.2 nm and 5.2 nm in O 0 2 respectively, which is 6.2 nm for 2H phase in O 40 -MoS 2 . However, 1 T MoS 2 is not stable and 1 T to 2H phase transition happens by annealing above 300 °C [15]. The S atoms may acquire enough energy to overcome the energy barrier and shift to the 2H phase sites [16].…”
Section: Methodsmentioning
confidence: 99%
“…8 Single and multilayer thin films of MoS 2 have interesting properties such as thickness-dependent band gap, 9 high carrier mobility, 10 large surface-to-volume-ratio, 11 strong spin-valley coupling, 12 chemical stability, and high mechanical flexibility. 13,14 The monolayer of MoS 2 shows a direct energy band gap ($ 1.9 eV), whereas the multilayer/bulk of MoS 2 shows an indirect band gap ($ 1.3 eV). 15 These properties make MoS 2 a promising material in future nanoscale electronic and optoelectronic device applications such as photocatalysis, 16 photodetectors, 17 biosensors, 18 gas sensors, 19 phototransistors, 20 field-effect transistors (FETs), 21 solar cells 22 and light-emitting diodes (LEDs).…”
Section: Introductionmentioning
confidence: 99%