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Retinal axial focusing and multi-layer imaging with a liquid crystal adaptive optics camera 下载免费PDF全文
With the help of adaptive optics(AO) technology, cellular level imaging of living human retina can be achieved.Aiming to reduce distressing feelings and to avoid potential drug induced diseases, we attempted to image retina with dilated pupil and froze accommodation without drugs. An optimized liquid crystal adaptive optics camera was adopted for retinal imaging. A novel eye stared system was used for stimulating accommodation and fixating imaging area. Illumination sources and imaging camera kept linkage for focusing and imaging different layers. Four subjects with diverse degree of myopia were imaged. Based on the optical properties of the human eye, the eye stared system reduced the defocus to less than the typical ocular depth of focus. In this way, the illumination light can be projected on certain retina layer precisely.Since that the defocus had been compensated by the eye stared system, the adopted 512 × 512 liquid crystal spatial light modulator(LC-SLM) corrector provided the crucial spatial fidelity to fully compensate high-order aberrations. The Strehl ratio of a subject with-8 diopter myopia was improved to 0.78, which was nearly close to diffraction-limited imaging. By finely adjusting the axial displacement of illumination sources and imaging camera, cone photoreceptors, blood vessels and nerve fiber layer were clearly imaged successfully. 相似文献
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This paper proposes a new Zernike modal gray map reconstruction algorithm used in the nematic liquid crystal adaptive optics system.Firstly,the new modal algorithm is described.Secondly,a single loop correction experiment was conducted,and it showed that the modal method has a higher precision in gray map reconstruction than the widely used slope method.Finally,the contrast close-loop correction experiment was conducted to correct static aberration in the laboratory.The experimental results showed that the average peak to valley (PV) and root mean square (RMS) of the wavefront corrected by mode method were reduced from 2.501λ (λ=633 nm) and 0.610λ to 0.0334λ and 0.00845λ,respectively.The corrected PV and RMS were much smaller than those of 0.173λ and 0.048λ by slope method.The Strehl ratio and modulation transfer function of the system corrected by mode method were much closer to diffraction limit than with slope method.These results indicate that the mode method can take good advantage of the large number of pixels of the liquid crystal corrector to realize high correction precision. 相似文献
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子孔径光学检测拼接准确度实验研究 总被引:2,自引:2,他引:0
实验研究了子孔径光学检测的拼接准确度.实验选取9个子孔径进行拼接,同时利用ZYGO干涉仪来测量子孔径和整个被检面的表面面形.实验发现,测量基准子孔径和整个被检面的时间间隔对子孔径拼接准确度的评价存在严重影响.为此,重点研究了产生影响的原因并提出了消除测量基准子孔径和整个被测面时间间隙影响的方法.最后,利用该方法研究了子孔径重叠面积对拼接准确度的影响.结果显示,当重叠面积比为7%时,PV和RMS的拼接误差分别为0.03λ(λ=632.8 nm) 和 0.01λ,并且重叠面积比和拼接准确度呈近似线性关系. 相似文献
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平行排列液晶器件的波前调制特性 总被引:18,自引:17,他引:1
设计了一种新型的平行排列液晶相位调制器(LC PM),可在纯相位的模式下进行相位调制,研究了液晶相位调制器的光学特性,理论上给予了分析.对畸变波前进行了调制,在1 cm2的校正面积上,调制后的准确度PV(peak to valley)值接近λ/15(λ=0.6328 μm),RMS(Root Means Square)可达到λ/100,斯特列尔比SR (Strehl Ratio)达到0.989.改变了传统的扭曲向列液晶器件难于进行纯相位调制和得到高准确度调制的缺点,达到了理想的效果. 相似文献
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液晶相位调制器的响应时间延迟是影响液晶自适应光学系统性能的一个主要因素, 为了提高系统的响应速度, 开发了一种快速响应的向列相液晶材料, 并制成了反射式硅基液晶器件(LCOS). 分析了该LCOS的相位调制特性及其对静态畸变波前和扰动波前的校正能力. 首先, 测量了LCOS的电光响应特性, 得出其780 nm相位调制量的响应时间为2 ms. 其次, 测量了LCOS的相位调制特性, 并对相位调制进行了线性化处理. 再次, 测量了用该LCOS搭建的液晶自适应光学系统的闭环和开环3 dB带宽, 它们分别为16和18 Hz. 最后, 给出了开环液晶自适应光学系统校正大气湍流的数值模拟结果, 结果表明. 系统的Strehl比由校正前的0.025上升到了校正后的0.225. 因此, 该液晶自适应光学系统可以对Greenwood频率为30 Hz以下的大气湍流进行较良好的校正. 相似文献
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高准确度LCOS自适应光学成像系统的研究 总被引:3,自引:0,他引:3
设计了一种液晶自适应光学成像系统.系统中高准确度硅基板液晶(LCOS)器件被用来校正波前位相.LCOS的优势在于它具有几十万个校正单元,而传统的变形镜最多只有1 000左右的校正单元,这种驱动单元的优势使LCOS拥有更高的校正准确度.系统中哈特曼波前传感器被用来测量波前畸变.对点光源进行闭环校正实验中,CCD相机获取了一个高清晰光点图像.实验中波前校正准确度为PV=0.08 λ,rms=0.015 λ(λ=632.8 nm),系统接近衍射极限. 相似文献
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研究了液晶分子排列对哈特曼波前探测器探测及闭环校正的影响.首先分析了分子排列对液晶校正器产生漏光强度的影响.详细探讨了在闭环校正过程中漏光对波前探测及校正准确度影响,当漏光比为40%时,产生的探测偏离误差为0.4;对于8%的漏光比,探测误差仅为0.08,可以忽略.最后分别做了扭曲和平行排列液晶校正器对静态畸变的闭环校正实验.对于漏光比为40%的扭曲液晶校正器,校正前后的PV和RMS值分别为:1.11 μm、0.25 μm和1.08 μm、 0.24 μm,说明漏光对闭环校正产生了严重影响.对于漏光比为8%的平行排列液晶校正器,通过闭环校正,波前的PV和RMS分别从1.58 m和0.22 m降到0.095 m和0.03 m,同时获得清晰的光纤束的像.结果表明,如果能够控制液晶波前校正器的漏光占总光强的比在8%以下,则可以获得高校正准确度. 相似文献