采样窗口对光学系统MTF测量影响的研究

对光学系统MTF测试中采样窗口对其测量影响进行了研究。在对标准镜头MTF测试时,采用离散傅里叶变换计算,线扩散函数扫描方向长度为所选针孔像线扩散函数半高宽的5倍左右时,MTF测试结果与设计值差异极值为0．011;采用快速傅里叶变换计算,线扩散函数扫描方向长度为所选针孔像线扩散函数半高宽的5倍左右时,同时采样点数要满足2^N,测试结果与设计值差异极值为0．010。为了证明此结论的普适性,按所提的采样窗口选取原则,对大像差镜头轴上和轴外的MTF进行了试验,并将测试结果与OPTIKOS的测试结果进行对比,最大极差为0．013。试验结果表明,此结论能够为光学系统MTF测试时采样窗口选择提供依据。     

Modified scaling angular spectrum method for numerical simulation in long-distance propagation

The angular method(AS)cannot be used in long-distance propagation because it produces severe numerical errors due to the sampling problem in the transfer function.Two ways can solve this problem in AS for long-distance propagation.One is zero-padding to make sure that the calculation window is wide enough,but it leads to a huge calculation burden.The other is a method called band-limited angular spectrum(BLAS),in which the transfer function is truncated and results in that the calculation accuracy decreases as the propagation distance increases.In this paper,a new method called modified scaling angular spectrum(MSAS)to solve the problem for long-distance propagation is proposed.A scaling factor is introduced in MSAS so that the sampling interval of the input plane can be adjusted arbitrarily unlike AS whose sampling interval is restricted by the detector’s pixel size.The sampling interval of the input plane is larger than the detector’s pixel size so the size of calculation window suitable for long-distance field propagation in the input plane is smaller than the size of the calculation window required by the zero-padding.Therefore,the method reduces the calculation redundancy and improves the calculation speed.The results from simulations and experiments show that MSAS has a good signal-to-noise ratio(SNR),and the calculation accuracy of MSAS is better than BLAS.     

光场强度分布测量中CCD噪声的校正北大核心CSCD

为了有效抑制CCD测量噪声带给激光对比度分布测量的影响,基于对比度测量模型,利用CCD测量噪声的先验知识及其输出观测值,给出了CCD噪声的校正方法。与现有计算方法的比较表明,该方法可以有效抑制CCD测量噪声带给测量的影响,其扩展不确定度从0.6%降低至0.3%,降低了测量不确定度,提高了测量的置信度。     

Bayer滤波型彩色相机调制传递函数测量方法

Bayer滤波型彩色相机广泛应用于航天遥感、空间对地观测、环境监测等领域.由于Bayer滤波片造成彩色相机相比黑白相机在像质方面进一步退化,如何对Bayer滤波型彩色相机成像性能全频段综合评价是目前亟待解决的问题.调制传递函数(MTF)是相机成像性能综合评价的关键指标,传统调制传递函数测量方法无法实现对Bayer滤波型彩色相机MTF全频段高精度测量.为了解决这个问题,本文提出了一种采用旋转刀口靶测量彩色相机调制传递函数的方法.理论方面,推导了Bayer滤波型彩色相机调制传递函数测量理论模型,仿真分析了刃函数采样率和刀口刃边倾斜角度误差对调制传递函数测量精度的影响,并给出了计算算法.实验方面,对彩色相机R,G,B三基色调制传递函数权重因子进行了实验定标,并搭建了基于条纹板和旋转刀口靶的彩色相机调制传递函数测量试验装置.采用旋转刀口靶法和条纹靶板法测量彩色相机MTF结果在耐奎斯特频率f_c处极差为0.061,在空间频率f_c/2处极差为0.043,试验结果验证了所提方法的有效性.     

一种基于针孔像分析的光学系统调制传递函数测量的自适应背景校正方法

提出了一种基于针孔像分析的光学系统调制传递函数(MTF)测量自适应背景校正的方法。由CCD显微系统采集针孔目标经被测光学系统成像后的针孔像,计算线扩展函数,并对其进行自适应背景校正,获取MTF。该方法与传统方法相比,消除了周围环境光照变化的影响,提高了测量精度。为验证所提方法的有效性,对标准镜头进行MTF测试,将测试结果与理论设计值比对,测试结果差异极大值为0.01;与美国Optikos公司的测试结果比对,测试结果差异极大值为0.015;对大像差光学系统的轴上和轴外进行MTF测试,并将测试结果与美国Optikos公司测试结果比对,测试结果差异极大值为0.013。实验表明,该方法可满足对不同像差光学系统轴上和轴外MTF的测量。     

光电经纬仪姿态测量精度室内检测方法

为实现光电经纬仪等靶场光测姿态测量设备测量精度的室内测试和评价,介绍了光电经纬仪对空间轴对称目标的姿态交会测量的原理。利用检测架、平行光管、目标轮廓靶及光源室内模拟不同姿态角的无穷远目标。建立了利用目标特征点的方位角、俯仰角计算目标姿态角的精确数学模型。用高精度经纬仪对目标上的多个特征点进行测量,用最小二乘法按该数学模型对目标姿态进行拟合,得到模拟目标的姿态,经验证该方法的标定精度可达0.05°。以该标定结果为模拟目标姿态的真值,光电经纬仪对同一模拟目标姿态进行动态测量,将测量结果与真值进行比较,可确定光电经纬仪的姿态测量精度。     

Broad-band phase retrieval method for transient radial shearing interference using chirp Z transform technique

The transient radial shearing interferometry technique based on fast Fourier transform (FFT) provides a means for the measurement of the wavefront phase of transient light field. However, which factors affect the spatial bandwidth of the wavefront phase measurement of this technology and how to achieve high-precision measurement of the broad-band transient wavefront phase are problems that need to be studied further. To this end, a theoretical model of phase-retrieved bandwidth of radial shearing interferometry is established in this paper. The influence of the spatial carrier frequency and the calculation window on phase-retrieved bandwidth is analyzed, and the optimal carrier frequency and calculation window are obtained. On this basis, a broad-band transient radial shearing interference phase-retrieval method based on chirp Z transform (CZT) is proposed, and the corresponding algorithm is given. Through theoretical simulation, a known phase is used to generate the interferogram and it is retrieved by the traditional method and the proposed method respectively. The residual wavefront RMS of the traditional method is 0.146λ, and it is 0.037λ for the proposed method, which manifests an improvement of accuracy by an order of magnitude. At the same time, different levels of signal-to-noise ratios (SNRs) from 50 dB to 10 dB of the interferogram are simulated, and the RMS of the residual wavefront is from 0.040λ to 0.066λ. In terms of experiments, an experimental verification device based on a phase-only spatial light modulator is built, and the known phase on the modulator is retrieved from the actual interferogram. The RMS of the residual wavefront retrieved through FFT is 0.112λ, and it decreases to 0.035λ through CZT. The experimental results verify the effectiveness of the method proposed in this paper. Furthermore, the method can be used in other types of spatial carrier frequency interference, such as lateral shearing interference, rotational shearing interference, flipping shearing interference, and four-wave shearing interference.