含负折射率介质非线性Bragg腔的双稳态特性

研究了含负折射率介质一维光子晶体非线性Bragg腔的透射特性、光学增强和双稳态特性.对负折射率介质无色散和有色散非线性Bragg腔及由两种正折射率介质构成的非线性Bragg腔的透射谱、光学增强、缺陷模的线宽、入射光的红移量、双稳态开关阈值进行了比较.含负折射率介质的非线性Bragg腔可显著增大腔内光学增强效应，降低缺陷模的线宽、入射光的红移量和双稳态开关阈值.     

Kerr缺陷一维耦合腔光波导的双稳态方向性

本文提出一种只在一层高折射率介质层中掺杂Kerr介质的一维耦合腔光波导.利用一维传输矩阵理论和非线性传输矩阵方法研究了此结构的光学双稳态.根据一维传输矩阵理论分析了此结构的线性特性,包括低频带边模的偏移及场分布的特点,讨论了此结构实现双稳态的原理.研究发现:由于缺陷层中场分布与入射光方向密切相关,而缺陷层光场的局域,将激发Kerr介质的三阶非线性效应,从而改变了缺陷层的折射率,所以不同方向的入射光具有不同的双稳态阈值.利用非线性传输矩阵方法研究了光学双稳态特性.结果表明:由于缺陷层的位置导致缺陷模正方向（由左到右）入射的场分布大于反方向（由右到左）入射的场分布,正方向的阈值低于反方向的阈值,相差一倍.     

非线性光学 位相共轭、自聚焦等相关效应

O437 2006043105含负折射率介质非线性Bragg腔的双稳态特性=Bistableproperties of nanlinear Bragg cavity containing negative re-fractive index materials[刊,中]/蒋美萍(南京理工大学材料科学与工程系.江苏,南京(210094)) ,陈光…∥光子学报.—2006 ,35(4) .—535-539研究了含负折射率介质一维光子晶体非线性Bragg腔的透射特性、光学增强和双稳态特性、对负折射率介质无色散和有色散非线性Bragg腔及由两种正折射率介质构成的非线性Bragg腔的透射谱、光学增强、缺陷模的线宽、入射光的红移量、双稳态开关阈值进行了比较。含负折射率…     

介质层厚对含负折射率介质Bragg微腔的影响

研究了介质层厚对含负折射率介质一维光子晶体Bragg微腔的缺陷模和双稳态的影响.在中心频率附近将传输矩阵各矩阵元采用泰勒级数展开并取一级近似,得到了缺陷模频率与介质层厚的关系式及品质因子公式.研究结果表明：一级近似法能很好地解释中心频率附近介质层厚对缺陷模频率的影响.理想Bragg微腔结构的缺陷模品质因子最大；递增正折射率介质层厚和增大缺陷层介质层厚、递减负折射率介质层厚及同时等量递减正和负折射率介质层厚,均可使缺陷模红移,双稳态阈值降低.     

非线性光学 非线性光学器件

O437 2006065109腔模红移对非线性微腔双稳态阈值的影响=Effects of red shifting in cavity-mode on the bistable threshold of nonlin- ear microcavity[刊．中]/沈小明(江苏工业学院信息科学系．江苏,常州(213013)),蒋美萍…//量子电子学报．—2006．23(3)．——413-415影响非线性微腔双稳态阈值的因素很多,例如电介质折射率、周期数、缺陷层厚度、谱线宽度等,但是腔模红移起到了十分重要的作用。从理论上分析了红移对双稳态阈值的影响。并作了数值模拟。图2参14(于晓光)     

Kerr缺陷一维耦合腔光波导的双稳态方向性

本文提出一种只在一层高折射率介质层中掺杂Kerr介质的一维耦合腔光波导.利用一维传输矩阵理论和非线性传输矩阵方法研究了此结构的光学双稳态.根据一维传输矩阵理论分析了此结构的线性特性,包括低频带边模的偏移及场分布的特点,讨论了此结构实现双稳态的原理.研究发现:由于缺陷层中场分布与入射光方向密切相关,而缺陷层光场的局域,将...     

一维三元光子晶体缺陷模的特性研究

在考虑色散关系的基础上,利用传输矩阵法讨论了一维三元光子晶体缺陷模的特征.结果表明:缺陷层几何厚度增加时,缺陷模中心红移,透射率下降,品质因子变小.三介质的几何厚度各自独立递增时,缺陷模都向长波方向移动,缺陷模的品质因子先增后降.入射角增大时,缺陷模中心蓝移,透射率不变,半峰全宽度变窄,品质因子变小.若忽略缺陷介质的色散,当其折射率减小时,缺陷模蓝移,透射率变大,半峰全宽度保持不变,品质因子增大.     

Kerr效应对二项式腔场谱量子干涉的影响

研究了含Kerr介质高Q腔内单个二能级原子与双模二项式光场发生双光子共振相互作用系统的腔场谱,给出了Kerr效应与量子干涉项ΔS(ω)关系的数值计算结果,讨论了Kerr效应对二项式腔场谱量子干涉的影响.结果表明:若初始时刻原子处于激发态而双模光场处于二项式态,随Kerr效应的增强,致使量子干涉项引起谱线强度的改变量呈现出"不规则的周期性衰减振荡"特性,震荡幅度与两模光场的频差密切相关.在Kerr系数χg(g为光场与原子的耦合常数)时,Kerr效应对干涉项的影响比较强烈;在χg时,趋于平稳.随着Kerr效应的增强,系统腔场谱由对称结构逐渐演化为不对称的多谱线结构.     

两模光场与原子相互作用中光场周期性和频效应-理想Kerr介质腔中非关联双模相干态光场与V型三能级原子相互作用系统中光场的不等阶和压缩效应

利用多模压缩态理论,通过数值计算研究了高Q Kerr介质腔中非关联双模相干态光场与V型三能级原子相互作用系统中双模光场的不等幂次高次和压缩效应,分别绘出了两模光场第一模i次方第二模j次方不等幂次和压缩度的第一正交分量(Sh1_ij),第二正交分量(Sh2_ij)的时间演化曲线.结果表明:1)Kerr介质的存在和嵌放在介质中的V型三能级原子是产生双模光场不等阶和压缩效应的物质条件,二者缺一不可.2)腔中光场和原子发生光子交换是导致双模光场不等幂次和压缩效应的微观机制.3)在不考虑坐标度的情况下,不同条件下的时间演化曲线呈现非常相似的"崩坍-复原-凹谷"式结构,且复原区的波型振荡次数及凹谷区的振荡下降和振荡上升型式一样.4)在χ以及,不变的条件下,不等幂次高次和压缩度时间演化曲线的崩坍-复原-凹谷式结构的持续时间随压缩阶次的升高而缩短,压缩度随压缩阶数的升高而迅速下降.5)在平均光子不变(即,恒定),但Kerr介质不同(即χ变化)的条件下,不等幂次高次和压缩度曲线的周期随Kerr介质的三阶非线性极化系数χ的增加而缩短,幅度则不受Kerr介质的三阶非线性极化系数变化的影响.6)不等幂次高次和压缩效应的持续时间等强烈地依赖于Kerr介质的非线性程度,χ越大不等阶和压缩效应持续时间就越短.在相同压缩幂次的情况下,不等幂次高次和压缩度演化曲线正向幅度随平均光子数的增大而增大.     

铷原子蒸汽中原子相干性导致的Kerr非线性增强效应及其应用研究

我们在理论和实验上研究了电磁感应透明对三能级Λ型Rb87原子蒸汽的Kerr非线性系数增强和减弱效应[1,2].用环型腔测量了Rb87原子的Kerr非线性折射率对耦合光强度、频率的依赖关系.发现当耦合光频率改变时,Rb87原子介质的Kerr非线性折射率将改变符号,并应用这一结果实现了腔内光场的开关控制.     

Low-threshold bistable reflection assisted by oscillating wave interaction with Kerr nonlinear medium

Owing to the enormously enhanced oscillating wave, a minute variation of the incident light intensity will give rise to a change in the dielectric constant of the Kerr nonlinear medium and lead to a bistable reflection with an ultra-low threshold intensity, which is closely related to the angle of incidence and the thickness of the Kerr nonlinear medium. The criterion for the existence of optical bistability is derived. Our bistability scheme is simple and not limited to the TM-polarization.     

Thickness dependent optical dispersion parameters and nonlinear optical properties of nanostructured Cr doped CdO thin films

Cr doped CdO thin films were deposited on glass substrates by reactive DC magnetron sputtering with varying film thickness from 250 to 400 nm. XRD studies reveal that the films exhibit cubic structure with preferred orientation along the (2 0 0) plane. The optical transmittance of the films decreases from 92 to 72%, whereas the optical energy band gap of the films decreased from 2.88 to 2.78 eV with increasing film thickness. The Wemple–DiDomenico single oscillator model has been used to evaluate the optical dispersion parameters such as dispersion energy (E_d), oscillator energy (E_o), static refractive index (n_o) and high frequency dielectric constant (ε_∞). The nonlinear optical parameters such as optical susceptibility (χ⁽¹⁾), third order nonlinear optical susceptibility (χ⁽³⁾) and nonlinear refractive index (n₂) of the films were also determined.     

水溶性CdTe量子点的三阶光学非线性极化特性

利用超短脉冲Z扫描技术和光学Kerr效应研究了以巯基丙酸为稳定剂的CdTe量子点水溶液的三阶光学非线性极化特性. 在532nm,30ps和800nm,130fs脉冲激光激发下, 发现分别具有正负相反取值的三阶光学非线性折射率,自由载流子吸收和双光子吸收分别是这两种脉冲激光激发下三阶光学非线性吸收的起因. 测量得到CdTe量子点的三阶光学非线性极化率约为CS₂的32倍, 在520—700nm光谱区的CdTe量子点的光学响应时间小于400fs. 关键词： CdTe量子点(QDs) Z扫描 三阶光学非线性极化特性 双光子吸收     

Experimental study on the chirped structure of the white-light continuum generation by femtosecond laser spectroscopy

The chirped structure of the white-light continuum generation (WLCG) pulse produced by focusing 800nm laser pulse with a pulse duration of 150fs (FWHM: full-width-at-half-maximum) onto a 2.4 mm thick sapphire plate was investigated by the optical Kerr gate technique with normal hexane as the optical Kerr gate medium. The observed WLCG was positively chirped, the measured anti-Stokes spectrum of WLCG ranges from 449 to 580nm with a temporal span of 2.56ps. When using metal reflecting mirrors to eliminate the group velocity dispersion (GVD) effect, we found that a span of 1.3ps still remained, indicating that the chirped pulse cannot be accounted for simply by GVD of the pulse propagation in the dispersive media. Our results suggest that the light-induced refractive index change due to the third-order nonlinear optical effect leads to an additional positive group velocity dispersion, which contributes to an important portion of the observed temporal broadening of the chirped WLCG. In addition to using reflective optical elements instead of dispersive optical elements, an effective way of reducing the chirp is to minimize the optical path length of the WLCG medium.     

基于157 nm激光制作的微光纤F-P折射率传感器

分析了157 nm激光制作的光纤法珀折射率传感器的传感特性.采用干涉条纹计数的方法对法珀腔的反射光谱进行解调,避免了光强波动的影响,同时具有较宽的折射率(RI)范围.在0~70℃范围内25 μm的法珀腔腔长变化量为6.25 nm,等效折射率变化为~2.46×10－4.常温下对折射率范围为1.33~1.427的甘油（丙三醇）溶液进行了测量,实验结果曲线的相关系数为0.9951,测量准确度为~3.70×10－4.     

Prospects for further threshold reduction in bistable microresonators

We discuss recent results showing the possibility of reducing further the switching threshold of GaAs quantum well bistable microresonators, taking into account the materials optical properties, both in the nonlinear medium and in the Bragg reflectors, as well as their departure from ideality, due to fabrication constraints. Threshold minimization in the presence of nonlinear index saturation is discussed, and the implications of this optimization on the geometrical design of bistable cavities are described. We present a new topographic technique for the assessment of the cavity resonance at various sample points. This technique is found to be very valuable for the characterization of the optical quality of epitaxial wafers grown for vertical cavity devices. Finally, we present some new approaches for the restriction of the lateral size of the device, and discuss the ultimate threshold reductions that can be expected from these considerations.     

Dispersive medium’s normal coupled modes and low threshold optical bistability in a symmetric one-dimensional photonic crystal

We present a detailed study of the dispersive medium’s normal coupled modes in a symmetric one-dimensional photonic crystals (1D PCs). The splitting, homogeneous broadening effect, and the detuning effect of the normal coupled modes can be well controlled by adjusting the parameters of the dispersive medium. The bistable behavior of the PCs with Kerr medium is also investigated and it is found that the threshold intensity of nonlinear optical bistability (OB) of 1D PCs with dispersive medium is much lower than that of structure without dispersive medium. The threshold intensity is strikingly sensitive to the coupling strength of the dispersive medium.