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消色差谱相位延迟器的光谱特性测试研究 总被引:5,自引:1,他引:5
本文应用归一化偏振调制原理建立的测试系统,对常规菲涅耳菱体,改进型菲涅菱体,斜入射型以及直角棱镜组合型的消色差相位延迟的光谱特性进行了测试研究,得到了各延迟器的消色差特性曲线,并对测试结果进行了分析。结果表明改进型菲涅耳菱体以及直色棱镜组合型型消色差相位延迟器,是目前较理想的实用型消色相位延迟器。 相似文献
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消色差相位延迟器的光谱特性测试研究 总被引:1,自引:0,他引:1
本文应用归一化偏振调制原理建立的测试系统 ,对常规菲涅耳菱体、改进型菲涅耳菱体、斜入射型以及直角棱镜组合型的消色差相位延迟器的光谱特性进行了测试研究 ,得到了各延迟器的消色差特性曲线 ,并对测试结果进行了分析。结果表明改进型菲涅耳菱体以及直角棱镜组合型消色差相位延迟器 ,是目前较理想的实用型消色差相位延迟器。 相似文献
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菱体型相位延迟器是高度消色差的λ/4相位延迟器.由于材料折射率色散的影响,在可见光范围内,仍存在2°的延迟偏差.为满足精确应用和测量的需求,从相位延迟的全反射相变理论出发,阐述了斜入射相位延迟原理,以菲涅耳菱体为例,分析了菱体型相位延迟器相位延迟随其入射角变化的规律性,结果表明:当光线非严格准直时,光的入射角对相位延迟量有明显的影响,延迟量不但对入射角变化敏感,而且还与入射光线的入射方位密切相关,呈不对称形式.当入射光的波长改变时,只需改变菱体延迟器的方位,让光线在菱体的前端面上斜入射,适当选取入射角,就可以补偿相位延迟的色散偏差,使同一菱体达到对不同波长都满足λ/4相位延迟.当角度调整精度Δi=±0.01°时,引入的延迟偏差不超过±0.009°,这一精度是其它石英波片或云母波片所不能比的. 相似文献
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根据菲涅尔全内反射相变理论,给出了双菱体λ/4消色差器的结构设计、性能分析和测量方法.由有效通光孔径和光线追迹设计出BK7玻璃在波长532 nm时相位延迟λ/4的双菱体的结构,用作532 nm至1 064 nm波长范围的标准λ/4相位延迟器.理论分析了入射角变化和波长变化对双菱体相位延迟的影响,当入射角变化限制在±4.3°以内时,其影响得到补偿;波长从532 nm到1 064 nm产生的误差为-0.65°.采用椭偏法中的消光技术,分别实测了双菱体在532 nm和1 064 nm波长下的相位延迟为:90.08±0.14°和88.99±0.1°,可知两不同波长产生的相位延迟误差为-1.09°. 相似文献
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液晶相位可变延迟器对光偏振态的调制 总被引:1,自引:5,他引:1
利用液晶相位可变延迟器(liquid crystal variable retarder, LCVR)的延迟相位随着其驱动电压连续可调特性,实现光偏振态的可控调制.设计了旋转检偏器,对LCVR进行820nm激光波长的现场校准,获得1/4λ、3/4λ和1/2λ、1λ相位延迟所对应的驱动电压,计算机控制其驱动电压实现对光偏振态的调制,并进行了检验,给出了理论分析和实验结果.该方法具有对光子入射方向不敏感、无需机械转动、适用较宽波长范围、实时可控等优点. 相似文献
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利用Jones矩阵法,理论上分析了方位角分别为0°和-45°的2个可变相位延迟器组成的偏振转换器可实现任意偏振态到水平线偏振态的转换,并推导出可变相位延迟器延迟量的表达式。利用自主研制的液晶相位可变延迟器的相位延迟,在1 V~2.7 V范围,根据驱动电压连续线性可调的特性,设计了两片液晶可变相位延迟器组成的偏振态转换器,实现了随机偏振态(Stokes参数为(-0.567,0.752,0.36))到水平偏振态(Stokes参数为(1,0,0))的可控调制,实验结果验证了理论分析结果。该偏振态转换器还可以实现其他任意偏振态到水平偏振态的调制。 相似文献
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光相位延迟量的归一化偏振调制测量 总被引:12,自引:7,他引:12
基于偏振调制原理,利用分束器代替检偏器,并从琼斯矩阵出发引入一归一化参数表征待测延迟量,提出了一种新的测量相位延迟量的方法,测量误差可小于0.8%。 相似文献
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Two-dimensional polarization distribution controller which can transform linearly polarized beam into two-dimensional polarization distributed beam has been presented and investigated. The two-dimensional polarization distribution controller consists of two quarter-wave plates and a variable retarder array. The principles of the two-dimensional polarization distribution controller are analyzed and calculated results show when the directions of fast axes of these three components meet a particular constraint equation set, these three optical components could be regarded as a two-dimensional polarization distribution controller. Experiments have been carried out, and the light intensity distribution of radially and azimuthally polarized beams after an analyzer are obtained. 相似文献
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本文介绍一种二次曝光合成狭缝彩虹消色象全息术,详细地分析了点源全息图的结构、消色象的分辨率和景深. 相似文献
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Large aperture phase-coded diffractive lens for achromatic and 16° field-of-view imaging with high efficiency 下载免费PDF全文
Diffractive lenses (DLs) can realize high-resolution imaging with light weight and compact size. Conventional DLs suffer large chromatic and off-axis aberrations, which significantly limits their practical applications. Although many achromatic methods have been proposed, most of them are used for designing small aperture DLs, which have low diffraction efficiencies. In the designing of diffractive achromatic lenses, increasing the aperture and improving the diffraction efficiency have become two of the most important design issues. Here, a novel phase-coded diffractive lens (PCDL) for achromatic imaging with a large aperture and high efficiency is proposed and demonstrated experimentally, and it also possesses wide field-of-view (FOV) imaging at the same time. The phase distribution of the conventional phase-type diffractive lens (DL) is coded with a cubic function to expand both the working bandwidth and the FOV of conventional DL. The proposed phase-type DL is fabricated by using the laser direct writing of grey-scale patterns for a PCDL of a diameter of 10 mm, a focal length of 100 mm, and a cubic phase coding parameter of 30π. Experimental results show that the working bandwidth and the FOV of the PCDL respectively reach 50 nm and 16° with over 8% focusing efficiency, which are in significant contrast to the counterparts of conventional DL and in good agreement with the theoretical predictions. This work provides a novel way for implementing the achromatic, wide FOV, and high-efficiency imaging with large aperture DL. 相似文献
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讨论了液晶相位可变延迟器(liquid crystal variable retarder, LCVR)在自旋极化电子产生方面的应用.LCVR控制入射光子的偏振度,从而实现对自旋极化电子束极化方向的调制.采用LCVR代替1/4波片和Pockels盒的优点在于其对入射光方向不敏感,传输直径大,不需要机械转动即可大波长范围的延迟,且易于校准.另外,还研制了旋转检偏器,通过示波器读出,对光子偏振性进行检测并对LCVR进行校准.
关键词:
自旋极化电子源
液晶相位可变延迟器
极化方向 相似文献
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高精度(Δ90°≤0.5″)长方体的制造技术主要包括了加工方法和检测方法两个方面,即长方体的前期加工阶段采用立方体(方砖)形式加工,以保证一个直角的精度;后期是采用分离器单块精抛的加工方式,以保证其平行差。加工过程中用Φ150激光平面干涉仪检测和控制面形及平行度,用LY Φ80棱镜干涉仪检测和控制直角精度。这种制造技术可以将长方体的直角精度做到Δ90°≤0 5″。 相似文献
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利用普通单模光纤(SMF)与色散补偿光纤(DCF)分别具有正色散和负色散系数特性,实现光纤光栅阵列的高速高精度解调.系统采用全光纤结构,仅需发出单一高速光脉冲,即可根据反射光脉冲时延差同时获取各个光栅的波长与位置信息,大幅提高了光纤光栅解调速度;通过建立DCF-SMF双通道和色散差矫正模型,削弱了温度变化及色散值误差对系统解调精度的影响.实验表明,本方法解调速率可达1 MHz,解调过程受传感网络光纤及双通道温变影响较小,具有良好稳定性及高精度;5—75?C温度扰动实验中,传感网络传输光纤温变时系统解调均方差16.8 pm,DCF-SMF双通道受温度扰动时系统解调均方差为11.9 pm,恒温下系统长时间解调时均方差为6.4 pm;应力实验中,解调线性度可达0.9998,解调精度约为8.5 pm. 相似文献
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多路激光打靶精度在惯性约束聚变实验中起着至关重要的作用,提出了基于X光针孔相机的激光打靶精度测试方法。根据显微镜读取的靶平面坐标系的靶孔中心坐标及打多孔靶后X光针孔相机所记录的靶孔中心坐标,建立靶平面坐标系和X光针孔相机坐标系之间的转换关系;通过打焦斑靶,建立焦斑模板,采用套模板的方法,读取X光针孔相机坐标系中焦斑中心坐标;由靶平面坐标系和X光针孔相机坐标系之间的转换关系,求出靶平面坐标系中焦斑中心坐标,计算得到激光打靶精度,分析打靶精度测试结果的不确定度,从而给出多路激光打靶精度测量技术和方法。 相似文献
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金属增强型反射镜在入射光非正入射的时候,两个不同的偏振态之间会产生不同的相移。利用最优技术设计了一种相位延迟器,其工作波长在640-670nm之间,入射角在40-50°范围内时,反射率>99%且相移为90°±20°。波长在670nm附近时相移对入射角不敏感。膜层厚度误差对相移影响最大。 相似文献
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To merge the beam from either of the two injectors to the main linac, a dog-leg system will be employed in the second Medium Energy Beam Transport (MEBT2) line of the China ADS driving accelerator. The achromatic condition has to be guaranteed to avoid beam center excursion against energy jitter. RF cavities were found to be indispensable to control the bunch length growth in the dog-leg system of MEBT2. The full uncoupling between transverse and longitudinal plane is desired to minimize the growth of projected rms emittances. The uncoupled achromatic condition of this dogleg system with the presence of RF bunching cavities will be deduced using the transfer matrices method. It is found that, to fulfill the uncoupling condition, the distance between the bunching cavities is uniquely determined by the maximum energy gain of the RF cavities. The theoretical analysis is verified by the simulation code TraceWin. The space charge effect on the uncoupled achromatic condition and the beam emittance growth will Mso be discussed. 相似文献