2013
DOI: 10.1021/nn405419h
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Valley Carrier Dynamics in Monolayer Molybdenum Disulfide from Helicity-Resolved Ultrafast Pump–Probe Spectroscopy

Abstract: We investigate the valley-related carrier dynamics in monolayer molybdenum disulfide using helicity-resolved nondegenerate ultrafast pump-probe spectroscopy at the vicinity of the high-symmetry K point under the temperature down to 78 K. Monolayer molybdenum disulfide shows remarkable transient reflection signals, in stark contrast to bilayer and bulk molybdenum disulfide due to the enhancement of many-body effect at reduced dimensionality. The helicity-resolved ultrafast time-resolved result shows that the va… Show more

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Cited by 231 publications
(249 citation statements)
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“…This value is in reasonable agreement with the value of τ s 7 ps estimated from PL experiments and with recent pump-probe measurements. 14,15 Similarly to the circular polarization degree whose decay is governed by τ zz , the linear polarization decay for the neutral A-exciton is governed by the in-plane pseudospin relaxation times τ xx and τ yy . As follows from Eq.…”
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confidence: 99%
“…This value is in reasonable agreement with the value of τ s 7 ps estimated from PL experiments and with recent pump-probe measurements. 14,15 Similarly to the circular polarization degree whose decay is governed by τ zz , the linear polarization decay for the neutral A-exciton is governed by the in-plane pseudospin relaxation times τ xx and τ yy . As follows from Eq.…”
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confidence: 99%
“…* e-mail: xdcui@hku.hk On the experimental side, however, the valley/spin lifetime of free carriers remains some ambiguity. A spin resolved photocurrent measurements estimated the valley/spin lifetime in the range of 10 0 ∼ 10 2 nanoseconds in monolayer WS 2 , while optical pump-probe spectroscopy and time-resolved photoluminescence (PL) experiments gave a very short valley lifetime of several picoseconds [16][17][18][19][20][21][22][23] with a few exceptions where long valley lifetime of bound excitons were reported. [24][25][26] The huge discrepancy lies in that the excitonic effect is prevalent in optical responses of monolayer TMDs.…”
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confidence: 99%
“…The energy shift is much larger compared to the quasi-2D systems like GaAs quantum wells. [16,43,44] To further study the valley dynamics in monolayer WSe 2 , we set the pumping energy to be 1.737 eV, which is resonant with the A exciton, and tune the probing energy in the range between 1.968 and 2.505 eV. The transient differential reflection at zero time delay are plotted as a function of the probing energy shown in FIG.…”
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confidence: 99%
“…2 A number of exciton decay mechanisms have been suggested as possible underlying processes in previously published studies [31][32][33][34][35][36][37][38][39][40][41][42][43] . For instance, some experiments 36,40 show that the fast decay dynamics (< 50 ps) are dependent on the exciton density and exciton-exciton annihilation is the dominating decay channel, while other studies 33,34,41 show no significant variation in the decay dynamics with the excitation density and that trapping by surface defect states is the responsible process. Other mechanisms such as carrier-phonon scattering, inter/intra-valley scattering, biexciton formation, trion formation, electron-hole recombination and exciton Auger scattering have also been considered 50 .…”
Section: Resultsmentioning
confidence: 99%