2017
DOI: 10.1007/s00339-017-0843-3
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The study of flexible emission and photoconductivity in 2D layered InSe toward an applicable 1000-nm light emitter and absorber

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Cited by 9 publications
(6 citation statements)
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“…Two major peaks obtained at 176 and 225 cm −1 are consistent with the E″ and A 1 ′ modes for the 2H phase InSe, respectively. 37,38 Two minor features observed at 198 and 237 ± 3 cm −1 are attributed to the A 2 ″(LO) and second-order A 1 ′ modes, respectively. By the curve fitting, the full width at half-maximum values of the two major Raman peaks are 10.2 (E″) and 8.2 (A 1 ′) cm −1 .…”
Section: Resultsmentioning
confidence: 99%
“…Two major peaks obtained at 176 and 225 cm −1 are consistent with the E″ and A 1 ′ modes for the 2H phase InSe, respectively. 37,38 Two minor features observed at 198 and 237 ± 3 cm −1 are attributed to the A 2 ″(LO) and second-order A 1 ′ modes, respectively. By the curve fitting, the full width at half-maximum values of the two major Raman peaks are 10.2 (E″) and 8.2 (A 1 ′) cm −1 .…”
Section: Resultsmentioning
confidence: 99%
“…The X feature is tentatively assigned to be associated with a deep ingap trap level which will be discussed in detail as below. Based on the previously reported PL studies [27][28][29][30], the L feature should be related to the bound shallow donor or acceptor state transition near P z orbital band edge, for which the strict optical transition selection rule for P z orbital can be relaxed owing to the bound carrier transitions of shallow donor or acceptor states. The PL spectroscopy of InSe flakes at RT is also measured, as shown in figure 1(d).…”
Section: Resultsmentioning
confidence: 99%
“…Since the electron-impurity and electron-defects scatterings are most likely present in our InSe flakes, the estimated electron-phonon coupling constant may differ from the real value. It is also noted that, the previously reported PL feature of InSe flakes was generally associated with impurities or defects [27,28,30]. The existing electron-impurity and electron-defects scatterings can largely affect the measured relaxation time so that the estimated electron-phonon coupling constant by only considering electron-phonon coupling becomes unreliable.…”
Section: Srhmentioning
confidence: 97%
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“…The value of the IF here larger than 2 may be caused by the existence of In or Se vacancies in InSe. [21,33] To understand whether the increased I d -V d forward current is because of graphene preventing carrier recombination between BP and InSe, we studied the excitation and recombination dynamics of BP, InSe, and the BP/G/InSe heterostructure using femtosecond-resolved transient absorption (TA) microspectroscopy (Figures S8 and S9, Supporting Information). [34][35][36] TA spectra for InSe showed an ultrafast photoinduced absorption (PIA) between 570 and 720 nm (Figure 2a) while BP displayed both PIA at 540-560 nm and photoinduced bleaching (PIB) at 520-530 nm (Figure 2b).…”
Section: Resultsmentioning
confidence: 99%