2014
DOI: 10.1021/jp4072197
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Observation of Ultrafast Carrier Dynamics and Phonon Relaxation of Graphene from the Deep-Ultraviolet to the Visible Region

Abstract: We investigated the ultrafast carrier dynamics and phonon relaxation of CVD-grown monolayer and 9-layer graphene on a quartz substrate. Excitation was performed at 400 and 800 nm. The normalized change in optical density ΔOD was probed over the range 260−640 nm (1.94−4.77 eV), reaching down into the region of graphene's Fano resonance, previously not investigated in femtosecond broadband pump−probe experiments. Time constants of 160 fs and 4 ps were found and assigned to carrier−optical phonon scattering and s… Show more

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Cited by 48 publications
(55 citation statements)
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“…22,38 There is a broad negative band appearing around 480 nm (partly obscured by the scattered pump light), and one notices the earliest portion of the build-up of a pronounced bleach band around 720 nm, i.e. A negative signal appears over the entire wavelength range.…”
Section: Ultrafast Perovskite Dynamics After Excitation At 500 Nmmentioning
confidence: 99%
See 1 more Smart Citation
“…22,38 There is a broad negative band appearing around 480 nm (partly obscured by the scattered pump light), and one notices the earliest portion of the build-up of a pronounced bleach band around 720 nm, i.e. A negative signal appears over the entire wavelength range.…”
Section: Ultrafast Perovskite Dynamics After Excitation At 500 Nmmentioning
confidence: 99%
“…Blue circles represent results for excitation at 500 nm (PSCP spectra in Fig. 22 Afterwards, the temperature decays more slowly, entering the regime where the decay of optical into acoustic phonons becomes important. Red circles are for excitation at 400 nm (PSCP spectra in Fig.…”
Section: Perovskite Dynamics Upon 400 Nm Excitationmentioning
confidence: 99%
“…Let us first remark that these quantities have been scarcely studied in the UV range [17][18][19] ; probably the most comprehensive study is that of Oum et al 19 . Roberts et al 18 suggest an intraband electron-electron scattering time τ e−e < 2 ps (the interband electron-electron scattering time has not been measured), followed by an electron-phonon intraband scattering time larger than τ 0 > 2 ps.…”
Section: Non-equilibrium Density-matrix and Bloch Equation In Thementioning
confidence: 99%
“…(12) to split the density into the equilibrium f c/v k and fluctuation ρ k parts, the susceptibility can be decomposed into an equilibrium χ 0 (q, ω) part, that is calculated using the equilibrium Fermi-Dirac distribution, and two pumped components, one intraband and the other interband, as: (19) where ω is the frequency of the probe. The intraband pumped component of the susceptibility reads…”
Section: Intraband Transitions Of the Non-equilibrium Gas Due Tomentioning
confidence: 99%
“…70 fs). [15] Thec ontour plots in Figure 3f or the change in optical density (DOD) after excitation with a4 00 nm pump pulse show that all three compounds switch upon irradiation. At early times (upper part), broad absorption appears near 600 nm and decays within ca.…”
mentioning
confidence: 94%