PPV衍生物的激发态动力学特性研究

利用共振飞秒光学克尔效应研究了C10－PPV溶液的非线性光学响应。实验结果表明，在共振激发条件下，C10－PPV挑学克尔效应信号表现为快速上升和随后的驰豫过程，其驰豫过程由两部分组成，一个200fs的快过程和一个400ps的慢过程。通过比较C10－PPV和掺杂C60后的C10－PPV荧光光谱，400ps的慢过程可归属为聚合物链内单重态激子在不同共轭段间的迁移过程。     

谐振式硅基二氧化硅集成光学陀螺的克尔噪声研究

分析了集成光学谐振式陀螺中克尔噪声的产生机理,利用导波光学理论建立了克尔噪声的数学模型,并基于此模型得出了克尔噪声对集成光学陀螺极限灵敏度影响的数学表达.分析了不同光源谱宽下谐振腔腔长与克尔噪声引起陀螺输出偏移之间的关系;针对集成光学陀螺中克尔噪声的主要产生原因-谐振腔中顺、逆时针的光强不均衡,仿真分析了系统中集成光学...     

不对称五氮齿大环金属配合物的光克尔效应

用飞秒脉冲激光作光源,利用泵浦－－探测方法测量了９个不对称五氮齿大环金属配合 物的时间分辨光克尔效应的响应信号,据此得到了它们的三阶光学非线性极化率ｘ＾（３）１１１１＝１．１９－３．３８×１０＾－１３ｅｓｕ和分子二阶超极化率γ１１１１＝８．０×１０＾－３２－２．８３×１０＾－３１ｅｓｕ以及光克尔效应响应不大于１６５ｆｓ等信息,讨论了周边取代基,中心金属离子和共轭π电子数对配合物三阶光学非线性极化率     

啁啾光脉冲在类时间透镜介质中的传播

利用空间－时间类似和光线光学方法得到啁啾高斯光脉冲在类时间透镜介质中传播的解析解，讨论了光脉冲宽度和啁啾参数随传播距离的演变，并与光脉冲在克尔介质中传播的特征作了比较。     

双折射光纤中克尔效应及光纤—光学逻辑门

本文详细地研究了单模双折射光纤中的克尔效应。讨论了其应用于光纤－光学逻辑门的优点，给出了有关的理论分析和计算结果以实验装置，确定了强度型逻辑门的“１／０”状态，测出了输出光脉冲宽度。理论分析和实验结果符合良好。     

电子-声子相互作用对柱形量子线中光学克尔效应的影响

本文利用密度矩阵方法研究了柱形量子线中的光学克尔效应, 重点讨论了电子-声子相互作用对其的影响,并以GaAs量子线为例进行了数值计算。结果显示,随着量子线半径R0的减小,光学克尔效应会逐渐增强;考虑了电子-声子相互作用时的光学克尔效应比未考虑电子-声子相互作用时的大20%多;量子线半径R0越小,峰越尖锐,峰值越强;当量子线半径R0大〖WTBZ〗于40 nm时,峰会逐渐消失.     

双折射光纤中克尔效应及光纤－光学逻辑门

本文详细地研究了单模双折射光纤中的克尔效应．讨论了其应用于光纤－光学逻辑门的优点,给出了有关的理论分析和计算结果以实验装置,确定了强度型逻辑门的“１／０”状态,测出了输出光脉冲宽度．理论分析和实验结果符合良好．     

附加克尔介质简并双光子J-C模型的动力学特性

本文利用密度算符间的距离研究了附加克尔介质简并双光子Jaynes－Cummings模型（JCM）的动力学特性．在与标准简并双光子Jaynes－Cummiungs模型以及附加克尔介质单光子Jaynes－Cummings模型相比较的基础上，详细讨论了克尔介质非线性相互作用对该模型动力学行为的影响．     

附加克尔介质Jaynes—Cummings模型的场熵演化

研究了附加克尔（Ｋｅｒｒ）介质Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ（Ｊ－Ｃ）模型场熵演化的动力学特性，讨论了克尔介质非线性相互作用以及失谐量对场熵演化的影响。     

基于瞬态光克尔效应的超快光学快门技术

系统介绍了几种基于瞬态光克尔效应的超快光学快门技术,包括传统的光克尔双折射快门技术,瞬态光栅快门技术,以及利用瞬态克尔透镜效应的光学快门技术。这些技术都是在泵浦-探测的实验配置基础上,利用门控光对克尔介质折射率的瞬态调制导致的信号光的相位（偏振态）、传播方向或光束发散角等光学特性的改变实现对信号光的超快时间分辨测量。对比讨论了这些超快快门技术的工作原理和实验配置,结果表明瞬态光束偏折快门技术相比其他快门技术具有无偏振配置要求、无相位匹配条件、超宽带光谱响应范围的特点,在光与物质相互作用的超快动力学研究中具有更为广阔的应用前景。     

基于光克尔门空间扫描单次激光信噪比测量

提出一种基于光克尔门空间扫描的单次激光信噪比测量方法.在该方法中,门光和探测光在光克尔介质中正交传输,通过光克尔门对探测光的空间扫描实现激光信噪比测量.采用该测量方法进行了单次激光信噪比测量的实验研究,测得时间窗口和分辨率分别为88.2ps、2.7ps.由于取样门是由光克尔效应来控制,因此该激光信噪比测量方法对于待测激光的波长没有限制.     

A nonlinear optical-fiber interferometer for nondemolitional measurement of photon number

A nondemolitional measurement scheme to determine the photon number was realised using an optical fiber as the optical Kerr medium. The φ⁽³⁾ value of an optical fiber for the optical Kerr effect was measured using this scheme. A classical correlation between the measured light intensity and the outgoing light intensity was observed experimentally. The goal of the measurement accuracy to obtain a quantum correlation is also discussed aiming at the quantum nondemolition (QND) measurement of the photon number.     

Spectral Hole Burning via Kerr Nonlinearity

Spectral hole burning is investigated in an optical medium in the presence of Doppler broadening and Kerr nonlinearity. The Kerr nonlinearity generates coherent hole burning in the absorption spectrum. The higher order Kerr nonlinearity enhances the typical lamb dip of the hole. Normal dispersion in the hole burning region while Steep anomalous dispersion between the two hole burning regions also enhances with higher order Kerr effect. A large phase shift creates large delay or advancement in the pulse propagation while no distortion is observed in the pulse. These results provide significant steps to improve optical memory, telecom devices, preservation of information and image quality.     

Spectral Hole Burning via Kerr Nonlinearity

Spectral hole burning is investigated in an optical medium in the presence of Doppler broadening and Kerr nonlinearity. The Kerr nonlinearity generates coherent hole burning in the absorption spectrum. The higher order Kerr nonlinearity enhances the typical lamb dip of the hole. Normal dispersion in the hole burning region while Steep anomalous dispersion between the two hole burning regions also enhances with higher order Kerr effect. A large phase shift creates large delay or advancement in the pulse propagation while no distortion is observed in the pulse. These results provide significant steps to improve optical memory, telecom devices, preservation of information and image quality.     

Stimulated rayleigh-kerr and raman-kerr scattering in a liquid-core hollow fiber system

By using a liquid-core multimode hollow fiber system with a long gain-length (2.5 or 7 m), a superbroadening stimulated scattering added to the pump line and/or the several orders of Stokes-stimulated Raman scattering lines of the core medium can be observed. This kind of stimulated scattering is related to the optical Kerr (reorientation) effect and Raman-induced Kerr effect in a liquid consisting of anisotropic molecules. Experimental studies of hollow fiber filled with different liquid samples (carbon disulfide, benzene, carbon tetrachloride) are reported. A theoretical approach based on a photon scattering model of optical Kerr effect and Raman-induced Kerr effect is proposed to explain the principal features of our experimental results. The significance of stimulated Kerr scattering studies and their potential applications are discussed.     

Controllable optical bistability of Bose—Einstein condensate in an optical cavity with Kerr medium

We study the optical bistability for a Bose-Einstein condensate of atoms in a driven optical cavity with Kerr medium. We find that both the threshold point of optical bistability transition and the width of optical bistability hysteresis can be controlled by appropriately adjusting the Kerr interaction between the photons. In particular, we show that the optical bistability will disappear when the Kerr interaction exceeds a critical value.     

Large Kerr effect in bulk Se-based chalcogenide glasses

High-speed optical communication requires ultrafast all-optical processing and switching capabilities. The Kerr nonlinearity, an ultrafast optical nonlinearity, is often used as the basic switching mechanism. A practical, small device that can be switched with ~1-pJ energies requires a large Kerr effect with minimal losses (both linear and nonlinear). We have investigated theoretically and experimentally a number of Se-based chalcogenide glasses. We have found a number of compounds with a Kerr nonlinearity hundreds of times larger than silica, making them excellent candidates for ultrafast all-optical devices.     

Controllable optical bistability of Bose-Einstein condensate in an optical cavity with a Kerr medium

We study the optical bistability for a Bose-Einstein condensate of atoms in a driven optical cavity with a Kerr medium. We find that both the threshold point of optical bistability transition and the width of optical bistability hysteresis can be controlled by appropriately adjusting the Kerr interaction between the photons. In particular, we show that the optical bistability will disappear when the Kerr interaction exceeds a critical value.     

Kerr-like nonlinearity induced via terahertz generation and the electro-optical effect in zinc blende crystals

A model is proposed to account for Kerr-like nonlinearity induced by femtosecond pulses via terahertz generation and electro-optical effect. This phenomenon, so far overlooked, is evidenced in a zinc blende single crystal with a heterodyne optical Kerr effect setup. The spectral evolution of this phenomenon as well as its noninstantaneous response character are reported. Its competition with a third-order optical Kerr effect is demonstrated.     

Longitude magneto optical Kerr effect of Fe/GaAs (0 0 1) with Al overlayers

The longitude magneto optical Kerr effect (LMOKE) is investigated on ultrathin Fe film grown on GaAs (0 0 1) substrate with Al overlayer. The formula of the longitude magneto optical Kerr effect is derived to find out the influence of the Al overlayer on the magneto optical properties of Fe/GaAs (0 0 1) sample. Results obtained from this formula fit very well with the experimental data. The change of the Kerr rotation as a function of the incident angle is also given, which can be used to find a proper angle in sample measurement. A numerical simulation was carried out to find out the relation between Kerr rotation and optical properties of the overlayer. Results from this simulation can be used to select the best overlayer material to protect the Fe/GaAs (0 0 1) sample.