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单根、双根和多根ZnO纳米棒中二次谐波产生与双光子诱导发光之间的竞争

Competition between second harmonic generation and two-photon-induced luminescence in single, double and multiple ZnO nanorods.

作者信息

Dai Jun, Zeng Jian-Hua, Lan Sheng, Wan Xia, Tie Shao-Long

机构信息

Laboratory of Nanophotonic Functional Materials and Devices, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, China.

出版信息

Opt Express. 2013 Apr 22;21(8):10025-38. doi: 10.1364/OE.21.010025.

Abstract

The nonlinear optical properties of single, double and multiple ZnO nanorods (NRs) were investigated by using a focused femtosecond (fs) laser beam. The excitation wavelength of the fs laser was intentionally chosen to be 754 nm at which the energy of two photons is slightly larger than that of the exciton ground state but smaller than the bandgap energy of ZnO. Second harmonic generation (SHG) or/and two-photon-induced luminescence (TPL) were observed and their dependences on excitation density were examined. For single ZnO NRs, only SHG was observed even at the highest excitation density we used in the experiments. The situation was changed when the joint point of two ZnO NRs perpendicular to each other was excited. In this case, TPL could be detected at low excitation densities and it increased rapidly with increasing excitation density. At the highest excitation density of ~15 MW/cm(2), the intensity of the TPL became comparable to that of the SHG. For an ensemble of ZnO NRs packed closely, a rapid increase of TPL with a slope of more than 7.0 and a gradual saturation of SHG with a slope of ~0.34 were found at high excitation densities. Consequently, the nonlinear response spectrum was eventually dominated by the TPL at high excitation densities and the SHG appeared to be very weak. We interpret this phenomenon by considering both the difference in electric field distribution and the effect of heat accumulation. It is suggested that the electric field enhancement in double and multiple NRs plays a crucial role in determining the nonlinear response of the NRs. In addition, the reduction in the bandgap energy induced by the heat accumulation effect also leads to the significant change in nonlinear response. This explanation is supported by the calculation of the electric field distribution using the discrete dipole approximation method and the simulation of temperature rise in different ZnO NRs based on the finite element method.

摘要

利用聚焦飞秒(fs)激光束研究了单根、双根和多根ZnO纳米棒(NRs)的非线性光学性质。特意将fs激光的激发波长选为754 nm,在此波长下,两个光子的能量略大于激子基态的能量,但小于ZnO的带隙能量。观察到了二次谐波产生(SHG)或/和双光子诱导发光(TPL),并研究了它们对激发密度的依赖性。对于单根ZnO纳米棒,即使在我们实验中使用的最高激发密度下,也仅观察到SHG。当相互垂直的两根ZnO纳米棒的连接点被激发时,情况发生了变化。在这种情况下,在低激发密度下可以检测到TPL,并且随着激发密度的增加而迅速增加。在约15 MW/cm(2)的最高激发密度下,TPL的强度变得与SHG的强度相当。对于紧密堆积的ZnO纳米棒集合,在高激发密度下发现TPL迅速增加,斜率超过7.0,而SHG逐渐饱和,斜率约为0.34。因此,在高激发密度下,非线性响应光谱最终由TPL主导,而SHG似乎非常微弱。我们通过考虑电场分布的差异和热积累的影响来解释这一现象。结果表明,双根和多根纳米棒中的电场增强在决定纳米棒的非线性响应中起着关键作用。此外,热积累效应引起的带隙能量降低也导致了非线性响应的显著变化。使用离散偶极近似方法计算电场分布以及基于有限元方法模拟不同ZnO纳米棒中的温度升高,支持了这一解释。

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