2000
DOI: 10.1016/s0022-2313(99)00291-4
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Creation of secondary excitons in solid Ar observed in the luminescence of molecular self-trapped excitons (M-STE)

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Cited by 2 publications
(2 citation statements)
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“…In Figs. 9 and 10, data are presented for Ar [24,31] and Ne [24]. In the case of Ar, the singlet component of the STE has been chosen as a fast decay channel for time-resolved excitation spectra (observation at 10.21 eV), in the case of Ne, the emissions of the atomic-type STE at 16.75 eV and of the so-called W-band at 15.5 eV were used for time-integrated measurements.…”
Section: The Special Case Of Argon and Neonmentioning
confidence: 99%
“…In Figs. 9 and 10, data are presented for Ar [24,31] and Ne [24]. In the case of Ar, the singlet component of the STE has been chosen as a fast decay channel for time-resolved excitation spectra (observation at 10.21 eV), in the case of Ne, the emissions of the atomic-type STE at 16.75 eV and of the so-called W-band at 15.5 eV were used for time-integrated measurements.…”
Section: The Special Case Of Argon and Neonmentioning
confidence: 99%
“…It made it possible to investigate recently the effects of exciton mixing in RGS and branched relaxation of electronic excitations. [2][3][4][5] But the measurement of excitation efficiency of free exciton luminescence within the absorption band of the lowest Γ(3/2) n = 1 excitons itself is attended by inevitable coincidence of the wavelength of exciting and emitting photons and usually it was not carried out in the experimental works. At the same time spatial and temporal fluctuation of the lattice potential caused by phonons and deformability of the lattice induce the broadening and existence of the low-energy tail of the excitonic absorption spectra and dressing of excitons by phonons, which leads to self-trapping of excitons.…”
Section: Introductionmentioning
confidence: 99%