TY - GEN
T1 - Exciton dynamics in the α-conjugated polymer of poly(di-n-hexylsilane)
AU - Suto, S.
AU - Shimizu, M.
AU - Goto, T.
N1 - Publisher Copyright:
© 1999 IEEE.
PY - 1999
Y1 - 1999
N2 - To elucidate the exciton dynamics at low exciton density, we have carried out measurements of the absorption, luminescence, luminescence excitation spectra, and time response of the luminescence intensity of poly(di-n-hexylsilane) (PDHS) film at 2 K. A broad absorption peak is observed at 3.40 eV and a sharp luminescence line at 3.37 eV. In the luminescence excitation spectra, the luminescence peak energy shift is found with the excitation energy below 3.385± 0.005 eV. This fact shows that the site selective excitation is observed below the excitation energy, and indicates that the energy relaxation rate of excitons changes dramatically around the energy. To understand the above results, we have formulated the exciton dynamics using a one dimensional Frenkel exciton Hamiltonian with disorder. We have also carried out measurements of the time response of luminescence intensity using the up-conversion technique in order to elucidate the exciton dynamics at high density. We have clearly observed the rise time of 1.4±0.5 ps, which is fifty times as fast as that at low exciton density. The decay time is also faster. Moreover, the luminescence quantum efficiency at the exciton density is ten times smaller than that at the low density. A process to explain these results is considered.
AB - To elucidate the exciton dynamics at low exciton density, we have carried out measurements of the absorption, luminescence, luminescence excitation spectra, and time response of the luminescence intensity of poly(di-n-hexylsilane) (PDHS) film at 2 K. A broad absorption peak is observed at 3.40 eV and a sharp luminescence line at 3.37 eV. In the luminescence excitation spectra, the luminescence peak energy shift is found with the excitation energy below 3.385± 0.005 eV. This fact shows that the site selective excitation is observed below the excitation energy, and indicates that the energy relaxation rate of excitons changes dramatically around the energy. To understand the above results, we have formulated the exciton dynamics using a one dimensional Frenkel exciton Hamiltonian with disorder. We have also carried out measurements of the time response of luminescence intensity using the up-conversion technique in order to elucidate the exciton dynamics at high density. We have clearly observed the rise time of 1.4±0.5 ps, which is fifty times as fast as that at low exciton density. The decay time is also faster. Moreover, the luminescence quantum efficiency at the exciton density is ten times smaller than that at the low density. A process to explain these results is considered.
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U2 - 10.1109/CLEOPR.1999.811646
DO - 10.1109/CLEOPR.1999.811646
M3 - Conference contribution
AN - SCOPUS:0033283739
T3 - CLEO/Pacific Rim 1999 - Pacific Rim Conference on Lasers and Electro-Optics
SP - 106
EP - 107
BT - CLEO/Pacific Rim 1999 - Pacific Rim Conference on Lasers and Electro-Optics
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 1999 Pacific Rim Conference on Lasers and Electro-Optics, CLEO/Pacific Rim 1999
Y2 - 30 August 1999 through 3 September 1999
ER -