2005
DOI: 10.1103/physrevb.71.115444
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Ultrafast photoresponse of metallic and semiconducting single-wall carbon nanotubes

Abstract: Utilizing a transient absorption ͑TA͒ technique based on a chirp-corrected broadband probe, we have studied the ultrafast photoresponse of dispersed HiPco single-wall carbon nanotubes ͑SWNTs͒ over the range of 440-1050 nm for excitation in the range of 430-1700 nm. While both metallic and semiconducting SWNTs show transient bleaching at their M 11 and S 11 energies for excitation above these energies, metallic SWNTs uniquely exhibit a photoresponse to sub-M 11 excitation. We observe a TA spectral response for … Show more

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Cited by 28 publications
(34 citation statements)
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“…The magnitude of the peak signals increases linearly with the fluence, as shown in the insets of semiconducting SWNTs. [16][17][18][19][20] This indicates that the photoinduced absorption we observed originates from the excitons in the second energy level. We attribute the short time constant to thermalization of the excitons.…”
mentioning
confidence: 70%
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“…The magnitude of the peak signals increases linearly with the fluence, as shown in the insets of semiconducting SWNTs. [16][17][18][19][20] This indicates that the photoinduced absorption we observed originates from the excitons in the second energy level. We attribute the short time constant to thermalization of the excitons.…”
mentioning
confidence: 70%
“…Photoemission 7 and transient absorption [8][9][10][11][12][13][14][15] transfer of excitons from semiconducting to metallic tubes. When such channels are eliminated in isolated tubes, the energy relaxation can take several picoseconds, [16][17][18][19][20] and exciton lifetimes of several 10 ps 17,18 to several 100 ps 16,19 have been measured. Time-resolved photoluminescence measurements have also shown decay times of several 10 ps.…”
mentioning
confidence: 99%
“…2(d) and 2(e) for various pump-probe delays . Transient transmission measurements with various pump-photon energies indicated that roughly half of the absorbed 1.6 eV photons excite the small-gap and metallic NTs [17]. Within 0.2 ps, the excited electrons relax to a Fermi-Dirac distribution f T with electronic temperature T [32].…”
Section: (D) Figures 2(d) and 2(e)mentioning
confidence: 99%
“…Atomic-force micrographs suggest a NT space-filling fraction F of $0:2. Roughly 2=3 of all NTs are large-gap tubes which become transparent at photon energies below 0.6 eV, whereas the small-gap and metallic NTs can still absorb photons [17].…”
mentioning
confidence: 99%
“…The spectrum is highly structured, consisting of a series of narrow induced absorption (IA) and induced transmission (IT) peaks, and stands in stark contrast to the broad and nondescript bands exhibited by many complex heterogeneous systems. We first reported this spectrum two years ago, 67,68 and since then, structured spectra have been observed by several other groups, [59][60][61][62]65,66 yet a clear explanation of its origin has not been identified. In this paper, we present evidence that the structured spectrum arises from a nonlinear optical response that causes a photoinduced red-shift in the exciton transition frequency when a second electron-hole pair is excited in the presence of an already existing exciton.…”
Section: Introductionmentioning
confidence: 99%