DocumentCode :
66671
Title :
Negative Slope for Second Harmonic Generation Observed at High Excitation Intensities in ZnO Nanorods
Author :
Jun Dai ; Qiao-Feng Dai ; Jian-Hua Zeng ; Sheng Lan ; Xia Wan ; Shao-Long Tie
Author_Institution :
Lab. of Nanophotonic Functional Mater. & Devices, South China Normal Univ., Guangzhou, China
Volume :
49
Issue :
11
fYear :
2013
fDate :
Nov. 2013
Firstpage :
903
Lastpage :
909
Abstract :
The nonlinear optical properties of ZnO nanorods (NRs) synthesized by coprecipitation method were investigated using a focused femtosecond laser light. The excitation wavelength was tuned from 750 to 795 nm so that excitons could be selectively generated via two-photon absorption above or below the exciton ground state of ZnO NRs. Both second harmonic generation (SHG) and two-photon-induced luminescence (TPL) were observed in the nonlinear response spectrum of ZnO NRs. The relative intensities of SHG and TPL were found to depend not only on excitation wavelength, but also on excitation intensity. At high excitation intensities, the nonlinear response spectrum became dominated by TPL for excitation wavelengths shorter than 770 nm, whereas it was still governed by SHG for excitation wavelengths longer than 770 nm. In addition, the intensities of SHG and TPL did not scale quadratically with excitation intensity but exhibited different slopes in different excitation intensity regimes, implying the existence of competition between them. More interestingly, a negative slope, which indicates a reduction of SHG with increasing excitation intensity, was observed at high excitation intensities for excitation wavelengths longer than 770 nm, implying the energy redistribution or energy transfer between SHG and TPL. Meanwhile, a slope much was identified for TPL at high excitation intensities. It is suggested that the reduction in the bandgap energy resulting from the effects of bandgap renormalization and temperature rise were responsible for the rapid increase of TPL. A weak exciton emission was resolved for excitation wavelengths longer than 770 nm and it was explained by the existence of Rabi oscillation.
Keywords :
II-VI semiconductors; energy gap; excitons; nanofabrication; nanorods; optical harmonic generation; photoluminescence; two-photon spectra; wide band gap semiconductors; zinc compounds; Rabi oscillation; SHG; TPL; ZnO; bandgap energy; bandgap renormalization; coprecipitation method; energy redistribution; energy transfer; excitation intensity dependence; excitation wavelength dependence; exciton emission; exciton ground state; excitons; focused femtosecond laser light; high excitation intensities; nanorods; negative slope; nonlinear optical properties; nonlinear response spectrum; second harmonic generation; temperature rise effects; two-photon absorption; two-photon-induced luminescence; wavelength 750 nm to 795 nm; Absorption; Excitons; Laser excitation; Nonlinear optics; Optical harmonic generation; Photonic band gap; Zinc oxide; ZnO nanorods (NRs); second harmonic generation (SHG); two-photon-induced luminescence (TPL);
fLanguage :
English
Journal_Title :
Quantum Electronics, IEEE Journal of
Publisher :
ieee
ISSN :
0018-9197
Type :
jour
DOI :
10.1109/JQE.2013.2275181
Filename :
6573346
Link To Document :
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