横向电光效应感应轴的确定

讨论了LiNbO3横向电光效应晶体的感应轴。横向电光效应有两种外加电场方式,虽然两种电光效应对晶体折射率和输出光强改变相同,但它们的感应轴方向却不相同。所以在光路的调节上就会有所不同。而且也可通过晶体的感应轴来确定晶体的xy轴。     

立方氮化硼横向电光调制半波电压的测量

宽禁带半导体材料立方氮化硼(cBN)具有闪锌矿结构和43m点群对称性,因此cBN晶体也是电光晶体。用cBN晶体进行了横向电光调制,首次观察到cBN的电光效应,并且测得了样品的半波电压．     

一种新的电光系数的测量方法研究

确定电光晶体的电光系数通常的方法是把电光晶体加工成规则的长方体进行测量.本文主要介绍如何对不规则形状立方氮化硼(cBN)晶体的电光系数的测量方法.cBN晶体是一种人工合成晶体,宏观点群对称性属于Td群,能够产生线性电光效应.但是合成的cBN晶体体积小,大约只有0.3mm×0.3mm×0.1mm,其硬度仅次于金刚石,不易将其加工成规则的长方体.根据cBN晶体的实际情况,进行理论推导,得到了适应于不规则形状的cBN晶体的线性电光系数的测量方法,并以此为指导,进行了实验测量,得到了cBN晶体的线性电光系数γ41=1.17×10-14m/V.     

双面电极下铌酸锂晶体中的电场分布及其应用——电控λ/2波片

晶体内部的电场分布是影响其电光特性的主要因素.采用有限元法分析了双面电极下铌酸锂晶体中的电场分布情况,讨论了晶体内部电场均匀分布区域与电极尺寸、晶体尺寸之间的关系.在此基础上,分析了光波在均匀电场中沿光轴传输时,铌酸锂晶体的双横向电光效应,得到了光波偏振方向与电场之间的关系,从而设计了一种适用于任意波长的电控λ/2波片.     

无源光纤脉冲电压电场传感器的研究

研究了一种利用电光晶体的一次电光效应测量脉冲电压和电场的方法,给出了光纤电压电场传感器的基本结构和测量原理,计算和对比了BGO和LN等几种不同晶体对测量灵敏度的影响.利用HP-8011A型脉冲信号发生器做为信号源,进行了初步的设计和测试,实验结果表明LN晶体具有较高的灵敏度、线性度以及较好的频率响应.     

无源光纤脉冲电压电场传感器的研究

研究了一种利用电光晶体的一次电光效应测量脉冲电压和电场的方法,给出了光纤电压电场传感器的基本结构和测量原理,计算和对比了ＢＧＯ和ＬＮ等几种不同晶体对测量灵敏度的影响,利用ＨＰ－８０１１Ａ型脉冲信号发生器做为信号源,进行了初步的设计和测试,实验结果表明：ＬＮ晶体具有较高的灵敏度,线性度以及较好的频率响应。     

3阶非线性效应对飞秒脉冲在掺镁铌酸锂晶体中时域延迟的影响分析

将3阶非线性效应引入至基于电光效应控制的超短脉冲群速度理论模拟研究:当改变输入光强、操作温度、波矢失配、极化周期以及横向直流电场时,2阶和3阶非线性效应的共同作用对超短脉冲在掺镁铌酸锂晶体中传播群速度的影响要明显大于仅考虑2阶非线性效应的作用效果.3阶非线性的引入进一步完善了基于块状晶体电光效应的偏振耦合效应,实现“慢光”方案的理论指导意义.     

锥光干涉图、光强透过率曲线对电光调制实验的影响

基于电光效应的基本原理,讨论了铌酸锂（LiNbO3）晶体横向电光调制实验中利用锥光干涉图暗十字线图样确定起偏器和检偏器偏振方向分别平行于晶体x,y光轴的方法,及光强透过率曲线偏移对测量铌酸锂晶体半波电压的影响．     

晶体的Pockels效应和电光张量

本文简要地介绍了晶体的普克尔效应和电光系数,强调指出电光系数是一个三阶张量,并进行了比较详细的讨论.     

准相位匹配PPKTP极化反转的监测

文中提出了采用电光效应实时监测判断KTiOPO_4(KTP)晶体周期性极化反转进程的实验方案,分析了在高压电场极化脉冲作用下,KTP晶体的电光效应的基本特性和极化电流所表现出来的峰值特性,以及它们与KTP晶体的铁电畴反转之间存在的依赖关系,并确定了用监控光强的变化来判断极化反转程度的基本依据,在监测系统的帮助下对熔盐法生长的KTP晶体进行了极化反转．最后对获得的PPKTP进行了化学蚀刻,结果表明,获得的PPKTP质量有了明显提高．倍频转换效率达到1．13%．     

BSO晶体(■■0)切面的二波耦合增益

考虑了压电和弹光效应对光波耦合的影响,在BSO晶体的(1 1 0)切面上,处理了矢量二波耦合问题,分别计算了入射光偏振态平行和垂直于入射面情况下的信号光的增益系数,得到了增益系数随光栅取向变化的函数关系.     

中心对称的对氨基苯甲酸-尿素超分子晶体的SHG效应

利用分子组装方法获得了对氨基苯甲酸/尿素超分子晶体，经X衍射单晶结构测定，晶体为中心对称结构，空间群为Pnab；经Nd；YAG皮秒激光器测试晶体粉末，以KDP粉末为参比，超分子晶体粉末的绿色倍频光的相对强度和积分值分别为80.20(KDP,176.40）和181.0（KDP，423.98），在超分子晶格中，尿素分子受到共存的对氨基苯甲酸分子的相互作用，改变了尿素分子在晶格中的彼此间的距离或取向，使中心对称的基态偶极矩的相互作用偏离最佳状态，能够部分地保持各自独立的超极化分张量，而呈现SHG效应。     

有机场效应管在晶体电光调制中的应用

利用以肽菁铜为半导体层的有机场效应晶体管构成一个 反向放大电路作为电光调制器的调制电路, 测试了其对光信号的调制效果. 实验结果表明, 有机场效应管在低频下可实现放大功能, 为电光晶体提供驱动和调制电压, 并实现了对激光信号的调制. 根据实验结果, 对该场效应管的性能进行了分析.     

PDLC制备及其电光性能测试实验

介绍聚合物分散液晶的工作原理以及聚合物分散液晶织构,通过实验给出液晶含量对聚合物分散液晶的形貌和电光性能的影响。该实验与课题组科研前沿内容相结合,内容新颖,直接与当代光开关等应用高科技相结合,对培养学生兴趣,开阔视野、启发思维都有促进作用。     

Orthogonally linear polarized lasers(Ⅰ)--principle and devices

Two kinds of orthogonally polarized lasers, i.e. Zeeman dual-frequency lasers and four-frequency ring lasers (laser gyros) have been developed since the invention of lasers, in which circularly polarized lights oscillate. This paper summarizes recent progress of the study on orthogonally linear polarized lasers with the standing wave cavity. Firstly, the expression of producing orthogonally linear polarized lights in standing wave cavity, i.e. laser frequency splitting, is given. Almost all the birefringence effects made in laser cavity are used to produce orthogonally linear polarized lights. The effect includes quartz crystal birefringence effect, calcite birefringence effect,stress (photo-elastic) birefringence effect and electro-optical birefringence effect. Secondly, several physical phenomena of orthogonally linear polarized lasers are discovered such as aberrance of frequency splitting curves caused by optical activity of quartz crystal, order-passing of longitudinal modes with frequency splitting and strong modes competition. Finally, because the traditional Zeeman dual frequency laser cannot output frequency difference larger than 3 MHz, the approaches of obtaining larger frequency difference are studied. The sequential results, several kinds of orthogonally polarized lasers, are described, such as birefringence dual frequency lasers outputting a frequency difference from 40 MHz to hundreds of megahertz, birefringence-Zeeman dual frequency lasers outputting a frequency difference from 1 MHz to hundreds of megahertz, the LD pumped YAG birefringence dual frequency laser outputting frequency difference of several gigahertz, and the lasers whose longitudinal mode spacing is c/4L instead of c/2L.     

Orthogonally linear polarized lasers (I) — principle and devices

Two kinds of orthogonally polarized lasers, i.e. Zeeman dual-frequency lasers and four-frequency ring lasers (laser gyros) have been developed since the invention of lasers, in which circularly polarized lights oscillate. This paper summarizes recent progress of the study on orthogonally linear polarized lasers with the standing wave cavity. Firstly, the expression of producing orthogonally linear polarized lights in standing wave cavity, i.e. laser frequency splitting, is given. Almost all the birefringence effects made in laser cavity are used to produce orthogonally linear polarized lights. The effect includes quartz crystal birefringence effect, calcite birefringence effect, stress (photo-elastic) birefringence effect and electro-optical birefringence effect. Secondly, several physical phenomena of orthogonally linear polarized lasers are discovered such as aberrance of frequency splitting curves caused by optical activity of quartz crystal, order-passing of longitudinal modes with frequency splitting and strong modes competition. Finally, because the traditional Zeeman dual frequency laser cannot output frequency difference larger than 3 MHz, the approaches of obtaining larger frequency difference are studied. The sequential results, several kinds of orthogonally polarized lasers, are described, such as birefringence dual frequency lasers outputting a frequency difference from 40 MHz to hundreds of megahertz, birefringence-Zeeman dual frequency lasers outputting a frequency difference from 1 MHz to hundreds of megahertz, the LD pumped YAG birefringence dual frequency laser outputting frequency difference of several gigahertz, and the lasers whose longitudinal mode spacing is c4L instead of c2L.     

Effect of pyrophosphate on the light scatter in KDP crystal

Pyrophosphate doped potassium dihydrogen phosphate (KDP) crystal was grown from aqueous solution by the temperature lowering method. Light scatter in KDP crystal was detected with the ultramicroscopic method. The light scatter in KDP crystal was aggravated when pyrophosphate was doped into the growth solution, which was distributed ununiformly in prism and pyramidal sectors of KDP crystal. Different effects of pyrophosphate on prism and pyramidal sectors of KDP crystal can explain this case. The transmission in this crystal was measured, showing that pyrophosphate affects the transmission evidently.     

初相移对电光双稳系统特性的影响

本文从带有延时反馈回路的电光双稳系统的动力学方程出发,研究了初相移对该系统的双稳态、非稳区域、稳区共振和非稳区频率锁定特性的影响。所得结果在其它类型的混合型延时反馈双稳系统中具有普遍性。     

大截面KDP晶体生长方法的初探

采用改变溶液PH值的方法研究溶液酸碱度对KDP晶体柱面生长的影响．当溶液的pH值在适当高的情况下对晶体柱面生长有利．另外，就大截面积KDP晶体生长方法进行初步探讨，为了得到大截面KDP籽晶，采用限制晶体的Z向生长是一种有效的方法．