Wenbin Peng, Qingxing Li, Zhenrui Yu, An Ning, X. Mai
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引用次数: 0
摘要
掺杂半导体微晶CdS x Se1- x(尺寸为10 nm - 100 nm)的玻璃由于其大的三阶非线性和快速的响应时间,最近引起了人们的广泛关注。Jain和Lind已经报道了在简并四波混频(DFWM)实验中测量到CdS x Se1- x掺杂玻璃的三阶非线性磁化率χ(8)为10-9-10-8 esu,并且非线性的起源可归因于短寿命电子空穴等离子体(带填充效应)的产生1。CdS x Se1- x掺杂玻璃的非线性响应约为3.5 ps2。因此,它在开发高速低功耗非线性光学器件方面具有很大的潜力。Junji Yumoto8使用含有CdS x Se1- x掺杂玻璃的外部法布里-珀罗(F-P)腔观察到了双稳性,双稳开关时间为25 ps。在本文中,我们报道了由CdS x Se1- x掺杂玻璃制成的内部F-P腔结构单模波导器件的光学双稳性。
Studies on the Dynanics of Optical Bistability Swithing in the Internal Fabry-Perot Cavity CdSxSe1-x-Doped Glass Waveguide Device
Glasses doped with semiconductor microcrystalline CdS
x
Se1-
x
(10 nm – 100 nm in dimension) have recently attracted muuch interest due to their large third-order nonlinearities and fast response times. Jain and Lind have been reported the third-order nonlinear susceptibilities χ(8) of CdS
x
Se1-
x
-doped glasses were measured to be 10-9–10-8 esu in a degenerate four-wave mixing (DFWM) experiment and that the origin of the nonlinearity can be attributed to the generation of a short-live electron-hole plasma (band-filling effect)1. The nonlinear response of CdS
x
Se1-
x
-doped glass has been got to be about 3.5 ps2. So it has great potential to be used in developing high-speed and low-power nonlinear optical devices. Junji Yumoto8 observed the optical bistablility made using an external Fabry-Perot (F-P) cavity containing CdS
x
Se1-
x
-doped glasses with bistable-switching time of 25 ps. In this paper we report the observation of optical bistability of an internal F-P cavity structure single-mode waveguide device made of CdS
x
Se1−x-doped glass.