Enhancement of third-order optical nonlinearity in effective epsilon-near-zero metamaterials of dielectric/metal/dielectric sandwich nanostructures

被引:0
|
作者
Tan, Jiaxing [1 ,2 ]
Liang, Shijie [1 ,2 ]
Qin, Xiaoqi [1 ,2 ]
Huo, Yanyan [1 ,2 ]
Lu, Heng [3 ]
Li, Jiangtao [3 ]
Zhao, Songqing [4 ]
Wang, Shuyun [1 ,2 ]
Ning, Tingyin [1 ,2 ]
机构
[1] Shandong Normal Univ, Shandong Prov Engn & Tech Ctr Light Manipulat, Jinan 250358, Peoples R China
[2] Shandong Normal Univ, Sch Phys & Elect, Shandong Prov Key Lab Opt & Photon Device, Jinan 250358, Peoples R China
[3] Chinese Acad Sci, Tech Inst Phys & Chem, Beijing 100190, Peoples R China
[4] China Univ Petr Beijing Karamay, Sch Arts & Sci, Karamay 834000, Peoples R China
基金
中国国家自然科学基金;
关键词
INDIUM TIN OXIDE; REFRACTIVE-INDEX; SUSCEPTIBILITY;
D O I
10.1063/5.0222019
中图分类号
O59 [应用物理学];
学科分类号
摘要
We report the enhancement of third-order optical nonlinearity in dielectric/metal/dielectric sandwiches driven by the epsilon-near-zero (ENZ) effect. The lithium niobate (LN) and Au are chosen as the typical dielectric and metal, respectively. The sandwich nanostructure consists of two layers of LN film (90 nm) and an insertion of Au layer of different thicknesses (9, 13, and 17 nm). The ENZ wavelength of LN/Au/LN (LAL) sandwiches is experimentally obtained with a modulation from 0.96 mu m (Au layer 17 nm) to 1.33 mu m (Au layer 9 nm). The nonlinear refractive index n(2) and nonlinear absorption coefficient beta are determined at variable near infrared wavelengths using the Z-scan method. The maximum n(2)=2.31x10(-14)(6.76x10(-15))m(2)/W and beta=-9.20x10(-8)(-1.94x10(-8))m/W are obtained in the LAL sandwich with a 13 nm Au layer of ENZ wavelength 1.088 mu m at the wavelength 1.064 mu m with a pulse duration of 25 ps (120 fs). The n(2) is around 19 and 25 times larger than those in the pure LN film of thickness 180 nm measured at the picosecond and femtosecond time domains, respectively. The enhancement of n(2) in LAL sandwiches follows the numerical results obtained from the ENZ effect. Especially, the LN layer and the Au layer have comparable contributions to the effective third-order susceptibility chi((3))(eff), which leads to the reconfigurable chi((3))(eff) by changing the thickness of each layer and further to modulate the n(2) and beta of the samples. The results offer a promising way to attain large and reconfigurable optical nonlinearities for application in all-optical photonic devices at a specified wavelength.
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页数:6
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