2016
DOI: 10.1063/1.4954837
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Well separated trion and neutral excitons on superacid treated MoS2 monolayers

Abstract: Developments in optoelectronics and spin-optronics based on transition metal dichalcogenide monolayers (MLs) need materials with efficient optical emission and well-defined transition energies. In as-exfoliated MoS2 MLs the photoluminescence (PL) spectra even at low temperature consists typically of broad, overlapping contributions from neutral, charged excitons (trions) and localized states. Here we show that in superacid treated MoS2 MLs the PL intensity increases by up to 60 times at room temperature. The n… Show more

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Cited by 62 publications
(78 citation statements)
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“…Note that various PL enhancement factors due to the TFSI treatment ranging from 60 to 190 have been reported, which depends on the quality of the MoS 2 monolayers. 20,34,46 Nevertheless, our result indicates that the defects in MoS 2 played an important role in the PL process. Even without the LSPR enhancement from Au NPs, the defects passivation in MoS 2 monolayers could have a notable enhancement effect.…”
Section: 3447mentioning
confidence: 59%
“…Note that various PL enhancement factors due to the TFSI treatment ranging from 60 to 190 have been reported, which depends on the quality of the MoS 2 monolayers. 20,34,46 Nevertheless, our result indicates that the defects in MoS 2 played an important role in the PL process. Even without the LSPR enhancement from Au NPs, the defects passivation in MoS 2 monolayers could have a notable enhancement effect.…”
Section: 3447mentioning
confidence: 59%
“…Figure a shows the fitting of the PL spectra at T = 173 K using four Voigt components. The most intense feature, named T A , is associated with the A trion . The strong intensity of T A is due to the excess of charge (possible optical doping) induced by the relatively high laser power used in our experiments .…”
Section: Resultsmentioning
confidence: 90%
“…The strong intensity of T A is due to the excess of charge (possible optical doping) induced by the relatively high laser power used in our experiments . The two smaller bands, better observed in Figure a, are named X A and X B and associated with the A and B excitons, respectively. The positions of T A , X A , and X B as a function of temperature are shown in Figure b and were fitted according to the equation: EX()T=EX()T=0+a()1+2exp()normalΘ/KBT, where E X ( T = 0) is the extrapolated band gap at 0 K, a is a fitting parameter, and Θ is an average phonon energy .…”
Section: Resultsmentioning
confidence: 99%
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“…23,24,29 For the SLM FET, such defects lead to various carrier mobilities, 19,24,[30][31][32][33] and defect repairing is the focus of concern during these years. 17,28,34,35 Here we report that a simple drop of chemical solution may repair the defect-rich SLM FET, by which the carrier mobility increases from 0.1 to around 30 cm 2 /Vs. The aberration-corrected high resolution transmission electron microscopy (HRTEM), Raman scattering, and density functional theory (DFT) calculations reveal the defect dynamics for the Selenium (Se) vacancy repair, which suggests the localization source of the transport carriers.…”
Section: Introductionmentioning
confidence: 81%