基因改性细菌视紫红质BR-D96N薄膜的偏振全息存储实验

采用透射式和反射式全息光路, 分别进行平行线偏振与正交线偏振记录, 对基因改性细菌视紫红质BR-D96N薄膜进行了偏振全息存储实验. 研究了两种偏振记录全息图的衍射光及散射光的偏振特性. 实验表明, 与平行偏振记录相比, 正交偏振记录可实现衍射光偏振状态与散射光偏振状态的分离, 易于滤除噪声, 提高读出图像的信噪比. 与用参考光再现相比, 用共轭参考光再现不仅能进一步提高再现图像的信噪比, 还能有效地消除记录物光路中位相物体引起的物光波前的畸变, 从而获得有较高保真度的再现图像. 此外, 在样品上进行了初步的角度复用体全息实验, 得到了无串扰、低噪声的结果.     

基于莫尔条纹实现体全息存储系统的准确寻址

利用光栅莫尔条纹实现角度多重体全息存储系统中精密移动平台的位移检测，有效地削弱该系统寻址的系统误差，提高了全息存储系统的数据读出的准确性．实验中在Fe：LiNbO3晶体中存储了300幅全息图，各幅全息光栅振幅不仅均匀性好，而且振幅相对较大。     

光折变全息图的热定影及H+数密度的影响

对Ce∶Fe∶LiNbO3晶体的体全息信息存储和热定影进行了理论和实验研究,从理论上分析了对不同空间频率的体全息图进行热定影所需的最小离子数密度,在国内首次对铌酸锂晶体中离子数密度进行了测试,并在不同的记录角度条件下进行了热定影实验,验证了理论分析的正确性.     

光折变体全息存储技术

磁存储和光盘存储是当今最主要的数据存储方式,但这种二维存储已不能满足人们对信息存储的要求.光折变体全息存储是最有前途的存储方式.介绍了光折变效应和体全息存储的基本原理,主要特点以及提高体全息存储容量的复用方法.     

基于共轭光再现技术的可擦写式全息光存储实验系统的优化

将一种生物光致变色材料——基因改性细菌视紫红质BR-D96N薄膜为记录样品,进行了共轭参考光再现可擦写式全息图像存储实验,并将其结果与参考光再现实验结果进行了比较.利用相同光路,还进行了透射式和反射式全息存储实验,并进行了比较.实验结果表明,反射式全息比透射式全息图记录可以获得高的信噪比,但衍射效率较低;共轭参考光再现可以实现对波前畸变的补偿,并且与参考光再现光路相比,共轭参考光再现可以实时监测衍射图像的形成及变化过程.通过记录光和读出光光强的调整(再现光光强约为物光或参考光光强的1/1000),可以消除读出的破坏效应.同时还证明,BR-D96N薄膜具有响应速度快,感光灵敏度高,擦写次数高,空间分辨率高,稳定耐用,使用方便等显著优点,非常适合作为一种动态全息或全息缓存记录介质.     

读出光对BSO类晶体中运动全息图衍射率的影响

研究了读出光对BSO类晶体中运动全息图衍射率的影响,指出读出光对BSO类晶体中运动全息图的衍射率有显著的降低作用。     

通过位相畸变介质的全息实时成象

本文介绍了一个新的实验,采用我们研制的Fe∶LiNbO_3晶体为记录介质,不需要两次通过位相畸变介质就能实时补偿透明物经过畸变介质后所产生的波前畸变。     

光折变晶体中写入阵列平面波导实验

进行了在光折变晶体中写入阵列平面光波导的实验研究,分别给出了在LiNbO3∶Fe晶体和SBN∶Cr晶体中写入阵列平面光波导的实验结果.实验结果表明,用这种方法写入阵列平面光波导简便可行.     

Fe∶LiNbO3晶体中全息图的选择性擦除研究

研究选择性擦除的原理和方法.针对铌酸锂晶体中定影全息图和未定影全息图的特点,介绍相应的选择性擦除的原理和在物光和参考光中引入π相位差的几种方法.通过引入π相位差记录互补全息图,利用全息图及其互补全息图的非相干叠加,消除原全息图对晶体折射率的调制,从而实现对未定影全息图的选择性擦除.实验中实现了在晶体中某一数据页面内部分数据的擦除,并从理论上对实验结果进行了分析.     

采秀光致折变晶体为记录介质的实时干涉测量

本文介绍采用光致折变晶体－－掺铁铌酸锂作为全息图记录介质实时干涉测量实验，结果表明这种晶体是一种替代全息干板的好材料，可以在实时干涉测量中广泛使用。     

光折变体全息存储研究

对光折变全息存储中的光折变效应、多重存储时复用编码技术作了论述 ,并提出了研究体全息存储的实验装置和串扰噪声的研究方法     

Holographic three-dimensional telepresence using large-area photorefractive polymer

Holography is a technique that is used to display objects or scenes in three dimensions. Such three-dimensional (3D) images, or holograms, can be seen with the unassisted eye and are very similar to how humans see the actual environment surrounding them. The concept of 3D telepresence, a real-time dynamic hologram depicting a scene occurring in a different location, has attracted considerable public interest since it was depicted in the original Star Wars film in 1977. However, the lack of sufficient computational power to produce realistic computer-generated holograms and the absence of large-area and dynamically updatable holographic recording media have prevented realization of the concept. Here we use a holographic stereographic technique and a photorefractive polymer material as the recording medium to demonstrate a holographic display that can refresh images every two seconds. A 50?Hz nanosecond pulsed laser is used to write the holographic pixels. Multicoloured holographic 3D images are produced by using angular multiplexing, and the full parallax display employs spatial multiplexing. 3D telepresence is demonstrated by taking multiple images from one location and transmitting the information via Ethernet to another location where the hologram is printed with the quasi-real-time dynamic 3D display. Further improvements could bring applications in telemedicine, prototyping, advertising, updatable 3D maps and entertainment.     

Diffraction property of photorefractive volume grating in Ce:KNSBN for ordinarily polarized reading beam

The diffraction efficiency of volume grating written by two wave mixing in Ce:KNSBN photorefractive crystal versus the writing beam ratio for ordinarily polarized reading beam is experimentally studied. The result is different from that for the extraordinarily polarized reading beam. Then the modified coupled-wave theory is used to fit the experimental data. The theoretical results are coincident with the experimental data quite well. This research gives a significant support to the applications of Ce:KNSBN crystal in holographic recording and optical information processing.     

体全息在共焦显微镜中的应用

采用体全息记录信息代替共焦显微镜中的反射镜,在物光的衍射光强最大的条件下,记录体全息信息.体全息共焦成像的动态范围取决于全息衍射效率和材料的限制,而深度分辨率则取决于物镜的数值孔径和记录介质的厚度大小.体全息共焦显微镜系统的观测结果对探测器前的光阑孔径大小没有明显的依赖关系,在探测器前加尺寸不必特别小的针孔或可以不加针孔,这样可减小由于衍射现象引起的像差.体全息成像本身具有滤波的作用.物镜的像差在体全息自成像过程中由于相位共轭而消除,从而使仪器的深度分辨率与测量的动态范围不再相互限制.     

Optical Property of LiNbO3 Crystal Codoped with In, Mg and Fe

In2O3, MgO and Fe2O3 were doped in LiNbO3 and Czochralski method was used to grow In:Mg:Fe:LiNbO3 crystals. The OH- extension transmission spectra, light scattering resistance ability, two wave coupled diffraction efficiency and response time of the crystal were measured. Codoping In and Mg in crystal will improve its light scattering resistance ability and response time. Doping In can increase the ability to replace antisite Nb and decrease the doping quantity of Mg. All these are propitious to improve the optical homogeneity of crystal. Doping Fe can improve the photorefractive sensitivity for LiNbO3 crystal. We discussed the site of In, Mg and Fe in LiNbO3 crystals and the influence of the absorption peak of OH- transmission spectra on photorefractive property for LiNbO3 crystal.     

Optical Property of LiNbO3 Crystal Codoped with In, Mg and Fe

In2O3, MgO and Fe2O3 were doped in LiNbO3 and Czochralski method was used to grow In:Mg:Fe:LiNbO3 crystals. The OH- extension transmission spectra, light scattering resistance ability, two wave coupled diffraction efficiency and response time of the crystal were measured. Codoping In and Mg in crystal will improve its light scattering resistance ability and response time. Doping In can increase the ability to replace antisite Nb and decrease the doping quantity of Mg. All these are propitious to improve the optical homogeneity of crystal. Doping Fe can improve the photorefractive sensitivity for LiNbO3 crystal. We discussed the site of In, Mg and Fe in LiNbO3 crystals and the influence of the absorption peak of OH- transmission spectra on photorefractive property for LiNbO3 crystal.     

The Effect of Oxidation／Reduction Disposing on Optical Properties of Mg： Fe： Mn： LiNbO3 Crystals

The congruent tri-doped Mg: Mn: Fe: LiNbO3 crystal has been grown by Czochralski method. Some crystal samples are reduced in Li2CO3 powder at 500℃ for 24 hours or oxidized for 10 hours at 1100 ℃ in Nb2O5 powder. Compared with As-grown Mg:Mn:Fe:LiNbO3, the absorption edge in UV-Vis. absorption spectrum of the oxidized sample and the reduced shifts to the violet and the red, respectively. Reduction increases the absorption of crystals in visible light region. In two-wave coupling experiments, the writing time, maximum diffraction efficiency and the erasure time of crystal samples in the same conditions are determined. The results indicate that oxidation and reduction disposing has great effect on the holographic recording properties of these crystals. The reduced crystal exhibits the fastest response time of 160 s anmng the crystal series. The mechanism of post-disposing effect on the holographic recording properties of Mg:Mn:Fe:LiNbO3 crystals are investigated.     

计算机辅助合成全息图

研究合成全息图的原理和记录方法。针对2D／3D合成全息图，分别讨论了对体视、动态、颜色和深度信息的编码以及全息观察窗的空间面积分割，计算了相关的记录参数．实验中采用计算机直接控制的液晶空间光调制器实现2D视差图像的自动显示与切换，方法简便易行，且消除了传统方法中底片复位所产生的误差，易实现自动化生产．实际制作了一个带有动感的合成彩虹全息图，验证了设计的正确性和方法的可行性．     

缝全息图象差研究

分析缝全息图象差的特性，指出全息图尺寸变化率和重现光与记录波长变化率对全息图象差的影响计算缝全息图象差的特性曲线，讨论消除和减少全息象差的条件．提出减少缝全息图象差的方法，给出实验结果     

Bleaching effect and nonvolatile holographic storage in doubly doped LiNbO<Subscript>3</Subscript>:Fe:Cu crystals

The bleaching effect, i. e. the crystal shows that decoloration after it is illuminated by ultraviolet light, has been observed in congruent LiNbO3:Fe :Cu crystals. Based on this bleaching effect, a new technique including the reco rding phase by two interfering red beams and fixing phase by both UV light and a coherent red beam has been experimentally investigated to realize nonvolatile holographic storage in LiNbO3:Fe:Cu. The results of proof-of-concept experiments confirm that bleaching effect becomes an alternative physical mechanism for nonv olatile holographic storage with high recording sensitivity and weak light-induced scattering noise.