Gap-Induced Giant Third-Order Optical Nonlinearity and Long Electron Relaxation Time in Random-Distributed Gold Nanorod Arrays

被引:14
作者
Wang, Xia [1 ]
Yao, Linhua [2 ,3 ]
Chen, Xiaodie [2 ,3 ]
Dai, Hongwei [2 ,3 ]
Wang, Mingshan [2 ,3 ]
Zhang, Luman [2 ,3 ]
Ni, Yun [1 ]
Xiao, Lixia [1 ]
Han, Jun-Bo [2 ,3 ]
机构
[1] Wenhua Coll, Sch Math & Phys, Wuhan 430074, Hubei, Peoples R China
[2] Huazhong Univ Sci & Technol, Wuhan Natl High Magnet Field Ctr, Wuhan 430074, Hubei, Peoples R China
[3] Huazhong Univ Sci & Technol, Sch Phys, Wuhan 430074, Hubei, Peoples R China
关键词
gold nanorods; surface plasmon resonance; local field enhancement; third-order optical nonlinearity; hot electron relaxations; AU TRIANGULAR NANOPRISM; 2ND-HARMONIC GENERATION; FANO RESONANCE; PLASMON RESONANCE; NON LINEARITY; ENHANCEMENT; DIPOLE;
D O I
10.1021/acsami.9b08935
中图分类号
TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
The third-order optical nonlinearities and the hot electron relaxation time (tau) of random-distributed gold nanorods arrays on glass (R-GNRA) have been investigated by using Z-scan and optical Kerr effect (OKE) techniques. Large third-order optical susceptibility (chi((3))) with the value of 2.5 x 10(-6) esu has been obtained around the plamsonic resonance peak under the excitation power intensity of 0.1 GW/cm(2). Further decrease of the excitation power intensity down to 0.3 MW/cm(2) will lead to the significant increase of chi((3)) up to 6.4 X 10(-4) esu. The OKE results show that the relaxation time of R-GNRA around the plasmonic peak is 13.9 +/- 0.4 ps, which is more than 4 times longer than those of the individual gold nanostructures distributed in water solutions. The Finite-difference time domain simulations demonstrate that this large enhancement of chi((3)) and slow down of tau are caused by the gap-induced large local field enhancement of GNRs dimers in R-GNRA. These significant results offer great opportunities for plasmonic nanostructures in applications of photonic and photocatalytic devices.
引用
收藏
页码:32469 / 32474
页数:6
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