共查询到16条相似文献,搜索用时 109 毫秒
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《中国光学与应用光学文摘》2006,(4)
O439 2006043796应用闭环残余倾斜数据分析自适应光学系统精跟踪回路性能=Performance analysis for fine tracking loop for a-daptive optical system with closed-loop residual tilt data[刊,中]/吴碧琳(中科院光电技术所.四川,成都(610029)) ,饶长辉…∥光学学报.—2006 ,26(4) .—487-490在自适应光学系统中,目标跟踪误差主要由未完全补偿的大气湍流扰动和望远镜抖放引起的跟踪误差以及系统的倾斜噪声误差两部分组成。提出一种用闭环残余倾斜数据计算倾斜噪声误差、大气湍流扰动和望远镜抖动引起的跟踪误差以及系统跟踪残余误差的新… 相似文献
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分析和介绍了自适应光学闭环系统中一种实用的实时多路自适应控制算法。该多路自适应控制算法综合考虑了大气湍流扰动以及自适应光学系统时间延迟对系统控制效果的影响,其各个控制回路的控制参数能根据外界扰动的变化进行实时的迭代调整,从而使系统始终工作在最优控制状态。利用61单元自适应光学系统上模拟的大气湍流扰动信号,实现了对变形镜各路控制电压进行闭环优化控制的多路自适应控制算法,并对该算法的收敛性、控制效果、控制带宽进行了仿真研究和分析。仿真结果表明,同经典比例积分控制算法相比,多路自适应控制算法具有更强的自适应性,可以更有效地减少外界扰动对自适应光学系统校正效果的影响,提高自适应光学系统的闭环控制带宽,改善控制特性。 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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自适应光学系统的控制残余方差分析 总被引:6,自引:4,他引:2
分析自适应光学系统的控制残余方差与控制带宽的关系.对于存在时间延迟的自适应光学系统,推导了计算大气湍流控制残余方差的近似方式,并给出了有探测噪声情况下确定系统最优控制带宽的公式.以61单元自适应光学系统为例,讨论了实验自适应光学系统中控制带宽的优化选择问题. 相似文献
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利用自适应光学系统的哈特曼(Hartmann)波前传感器,测量了激光实际大气水平舆湍流畸变波前中整体倾斜像差的时间功率谱,发现功率谱谱形与科尔莫戈罗夫(Kolmogorov)湍流理论不完全符合,建立了一种根据实际测量的整体倾斜功率谱估测自适应光学系统斜镜需要的控制带宽大小和大气湍流的泰勒(Tyler)频率指标的方法。 相似文献
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Mohammad Moradi 《Optical Review》2008,15(2):125-129
The goal of this study was to analyse anisoplanatism of adaptive optics under an inhomogeneous turbulent atmosphere over a
pupil of finite size. By means of a numerical model with layers of turbulence software was proposed by which point spread
function (PSF), optical transfer function (OTF) as well as system isoplanatic angle can be calculated. Atmospheric turbulence
was simulated with the aid of a set of moving random phase screens with arbitrary statistics. Both reference and target are
assumed to be the point light sources. To simulate atmospheric turbulence we applied the concept of a number of moving random
phase screens with Kolmogorov spectrum. In my investigation I used the model of the Shack-Hartmann wave front sensor and the
ideal model of a wave front adaptive mirror that is assumed to reproduce a given number of Zernike polynomials without time
delays. The designed software allows calculation of instantaneous and average values of phase correction errors at different
angles between a reference beacon and target source. Simulations can be made with a broad range of parameters of an adaptive
system and atmospheric turbulence. The system of the model allows changing of the control algorithm of phase correction. Both
common phase conjugation and weighted phase conjugation algorithm have been tested. This program is capable of calculating
the effects of beam diffraction during propagation in the atmosphere. 相似文献
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Modal prediction for closed-loop adaptive optics 总被引:1,自引:0,他引:1
The correction efficiency of adaptive optics is limited mainly by measurement noise and time delay. To overcome this problem, we describe a new modal linear predictive controller whose parameters are optimized by means of a recursive least-squares algorithm to minimize the residual optical phase variance. The method copes with the recursivity of the closed-loop operation. We demonstrate that the optimal rejection transfer function for adaptive optics is proportional to the frequency signal-to-noise ratio. Finally, we present what we believe to be the first experimental results obtained with a predictor used to control the tip-tilt mirror of an adaptive-optics system. 相似文献
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A closed-loop adaptive optics system based on a self-referencing interferometer wavefront sensor (SRI WFS) using phase-shifting point-diffraction technique and an electrically addressed phase-only liquid-crystal spatial light modulator (LC SLM) is built and validated experimentally. The wavefront aberration of incoming beam is directly measured by analyzing four frames phase-shifted interferograms captured by a single CCD camera in two camera shots, and then by loading the conjugate function onto the SLM the wavefront aberration is corrected. The proposed scheme does not rely on any complicated control algorithm or wavefront-reconstruction algorithm and can achieve high-resolution and high-accuracy correction. Closed-loop correction results of single order Zernike aberrations and a Kolmogorov turbulence phase screen show that considerable improvements in the Strehl ratio (of greater than 0.94) is achieved. 相似文献
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Quanquan Mu Zhaoliang Cao Zenghui Peng Lifa Hu Li Xuan 《Optics Communications》2010,283(10):2017-2019
The adaptive optics system (AOS) often operates in a discrete sampling process with finite closed-loop frequency. Reconstruction, detection, and time lag induced errors are the main correction errors of the system. An AOS that is based on a liquid crystal (LC) benefits from the LC’s high correction precision, thus the reconstruction error can be ignored. The primary error will be induced by the time lag from the time of detection to the time of compensation. In this paper, some theoretical simulations are introduced in order to evaluate the correction precision of AOS with an LC corrector. The main purpose is to compare the correction precision between the open-loop and closed-loop control. We attempt to find a method to ascertain the exact precision of the open-loop control and show whether it improves the correction precision. The conclusion is thus reached that the actual error rejection bandwidth for the closed-loop was lower than the −3 dB error rejection bandwidth measured in practice. The increased refresh frequency of the open-loop control can improve the imaging performance to nearly −3 dB bandwidth of the detector measured, which is the maximum possible bandwidth due to the time lag. 相似文献