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庞志海樊学武马臻邹刚毅 《光学学报》2016,(5):202-208
利用条纹泽尼克多项式来表征自由曲面的光学元件,并将多项式中表示初级球差、彗差、像散项转换为矢量形式.利用矢量波像差理论,研究了自由曲面光学元件校正光学系统初级像差的特性.通过分析可知,自由曲面在光学系统中不同位置时所校正的像差特性不同.当自由曲面位于光学系统的孔径光阑(入瞳或出瞳)上可以校正光学系统全视场内为常数的初级像差;当自由曲面远离孔径光阑时,由于轴外视场成像光束口径的缩放与偏移,自由曲面可以校正非对称初级像差,且不同初级像差与视场依据关系不同. 相似文献
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Dipankar Bhattacharyya Ayan Ray Bibhas K. Dutta Pradip N. Ghosh 《Optics & Laser Technology》2002,34(1):93-96
It is shown that Fizeau interferometry provides an accurate optical method to measure the refractive index and wedge angle of transparent plates used as optical components in different experiments. A near IR external cavity diode laser having spectral resolution up to 10−7 has been employed to measure the refractive index of the test plates by introducing amplitude modulation technique in the detection system of our phase shifting Fizeau interferometry. Detection of spatial fringes has been performed to find out the wedge angles of the plates by using a He–Ne laser along with the CCD-image sensor. 相似文献
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本文系统地研究了由玻璃与液晶构成的非线性光学界面。用一台调Q的红宝石激光器研究了由玻璃与处于各向同性液相的液晶所构成的非线性界面。在不同入射角时非线性界面由内部全反射跃变到部分透射的阈值光强与Kaplen的平面波理论计算结果相一致。在T-Tc=2.5℃条件下测量了时间分辨的非线性界面的反射率。观察到了反射率的滞后迴线。非线性界面的这种反射率的滞后迴线可以归之于液晶分子退取向的弛豫过程。用Ar+激光器研究了玻璃与向列相液晶所构成的非线性光学界面,观察到了由相变而产
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激光束照射到表面被粘污的反射镜上会产生干涉环,入射光束和反射光束在被粘污表面产生散射光干涉.随着入射角的变化,光束在反射镜玻璃片内光程改变,引起干涉环从中心冒出或缩进,干涉环级数的变化与入射角的平方成正比. 相似文献
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波前编码系统相位板视场效应的消除 总被引:2,自引:2,他引:0
通过在光学系统的光阑面上加入一个非球面相位板,使得光学系统的成像对离焦不敏感.但当入射视场角较大时,图像的边缘发生变形且难以恢复.针对此问题,提出了两种解决方案,方案一是把相位板移至光路中光线较为平缓的区域,但不是系统的光阑位置;方案二是保持相位板位置不变,优化整个光学系统,使相位板前的光线能够平缓地入射到相位板.实验中对一个EFL=12.5 mm,F/#=1.3,半视场角为13.5°的波前编码实际系统进行仿真比较,得出方案二可以有效地消除波前编码相位板引入的视场效应. 相似文献
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A. Morinaga F. Riehle J. Ishikawa J. Helmcke 《Applied physics. B, Lasers and optics》1989,48(2):165-171
An optical frequency standard based on frequency stabilization to Ramsey fringes observed in a Ca atomic beam is described. The important operation parameters influencing the uncertainty of such a standard are studied experimentally. Frequency shifts due to phase errors of separated traveling wave excitation can be strongly reduced by means of laser beam reversal. It is expected that the present fractional uncertainty of approximately 2.3×10–12 to realize the true line center can be reduced below the 10–14 level by applying atomic beam cooling and improved phase alignment. 相似文献
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Optical transfer function analysis of circular-pupil wavefront coding systems with separable phase masks 下载免费PDF全文
This paper proposes a simple method to achieve the optical transfer function of a circular pupil wavefront coding system with a separable phase mask in Cartesian coordinates.Based on the stationary phase method,the optical transfer function of the circular pupil system can be easily obtained from the optical transfer function of the rectangular pupil system by modifying the cut-off frequency and the on-axial modulation transfer function.Finally,a system with a cubic phase mask is used as an example to illustrate the way to achieve the optical transfer function of the circular pupil system from the rectangular pupil system. 相似文献
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Optical interference fringes were observed in the beam spot of the He-Ne laser transmitted through KDP. The interference fringes originate from the dynamic gratings induced by the electromagnetic field of the incident light. Diffraction fringes appear only in certain propagation directions of light through KDP. This observation is different from that monitored in α-quartz. 相似文献
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我们研制的地基气辉成像干涉仪(ground based airglow imaging interferometer,GBAⅡ)样机成功地探测了地球上空90—100 km的大气风速和温度.为了提高GBAⅡ的探测精度,本文研究GBAⅡ所拍摄的成像干涉条纹的定标:对干涉条纹中心位置定标、电荷耦合器(CCD)暗噪声和平场定标、整个光学系统衰减系数定标、步进步长定标、光程差随入射角变化量定标、仪器响应度定标和零风速相位定标等理论和实验进行了研究.利用最小二乘法对GBAⅡ拍摄的30幅成像干涉图的圆心坐标定标在CCD(123.3,121.1)像素位置;利用632.8 nm激光获得GBAⅡ所用CCD的平场定标系数矩阵,分别得到平场前后的干涉图并检测出CCD的噪声和坏点;利用GBAⅡ获得图像的边缘亮环相位与中心亮斑相位的差值对入射角10.24°时,光程差相对0°入射角时变化了0.356个条纹;拍摄200幅成像干涉图的实验离散点进行正弦拟合后的均方根标准偏差达90.34%,该完整干涉条纹的步进间隔为4.06 nm,对应步进相位为0.0094π;针对正演公式中GBAⅡ的系统衰减系数对所拍摄的原始干涉图利用IDL编程得到光学系统衰减系数的多项式,拟合的均方根标准偏差达99.98%;采用632.8 nm激光作光源,简化了GBAⅡ的响应度表达式,通过实验得其响应度为4.97×10~(-3)counts·(Rayleigh·s)~(-1);针对GBAⅡ室外观测,给出零风速定标的矩阵表达式后,对532.0 nm和632.8 nm激光的对应零风速相位分别为-9.2442°和-68.6353°.本文提供了多种定标方法,并逐一通过实验进行验证,为国内被动遥感探测高层大气风场提供了强有力的实验支持. 相似文献