2019
DOI: 10.1063/1.5115467
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Ultrafast carrier and phonon dynamics in few-layer 2H–MoTe2

Abstract: By using femtosecond pump-probe spectroscopy with broadband detection from near-infrared to midinfrared, the carrier and phonon dynamics in few-layer 2H–MoTe2 after ultrafast excitation have been investigated in detail. Immediately following the photoexcitation, an ultrafast relaxation of the generated hot carriers by releasing phonons is observed within hundreds of femtoseconds. The subsequent electron-hole recombination with a time constant of ∼1.5 ps is clearly identified and demonstrated to be mediated thr… Show more

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Cited by 32 publications
(40 citation statements)
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“…33 – 35 ). The measured changes in the mid-infrared (MIR) region were mainly caused by the absorption of photogenerated carriers 73 , 74 . We fitted the decay kinetics of photogenerated carriers using a second-order exponential fit, where τ 1 indicates that the photogenerated carrier is rapidly compounded after exciton dissociation and τ 2 indicates that the photogenerated carrier is trapped during migration after dissociation (Supplementary Note 5 ).…”
Section: Resultsmentioning
confidence: 99%
“…33 – 35 ). The measured changes in the mid-infrared (MIR) region were mainly caused by the absorption of photogenerated carriers 73 , 74 . We fitted the decay kinetics of photogenerated carriers using a second-order exponential fit, where τ 1 indicates that the photogenerated carrier is rapidly compounded after exciton dissociation and τ 2 indicates that the photogenerated carrier is trapped during migration after dissociation (Supplementary Note 5 ).…”
Section: Resultsmentioning
confidence: 99%
“…[ 33 ] In sharp contrast, the phonon bottleneck effect at a high pump fluence may severely limit the hot carrier cooling rate and slow down the build‐up of band‐edge excitons (see Figure S5b , Supporting Information). [ 33 , 58 ]…”
Section: Resultsmentioning
confidence: 99%
“…The time-resolved photoluminescence (TRPL) decay curve (Figure 2b) shows a near-perfect single-exponential decay with a lifetime t = 22.2±0.1 ns that is four orders of magnitude longer than that in pristine MoTe 2 (~2 ps), which is attributed to the non-radiative decay dominated process. 23 This long lifetime provides a clear indication that localization of the exciton in a strain induced potential trap prevents the exciton from recombining via non-radiative defects that dominate the decay of 2D band-edge excitons.…”
mentioning
confidence: 99%