CN114964522A - Hartmann wavefront restoration method based on pupil mapping model - Google Patents
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Abstract
本发明提供一种基于光瞳映射模型的哈特曼波前复原方法,根据哈特曼波前传感器的入射光瞳信息,通过数据处理方式,提取光瞳分布的时域/空域非均匀性特性导致的子孔径质心偏差,选择质心偏差小的子孔径,通过重构模式复原矩阵的形式完成波前复原。该方法综合考虑了光瞳的非均匀特性,尤其适于具备动态强度分布特性光瞳的哈特曼波前探测。同时,对动态强度分布光瞳下的像差准确校正、多校正器稳定解耦等方面也可提供一定的辅助作用。
The invention provides a Hartmann wavefront restoration method based on a pupil mapping model. According to the incident pupil information of the Hartmann wavefront sensor, the time domain/spatial domain non-uniformity characteristics of the pupil distribution are extracted through data processing. The resulting sub-aperture centroid deviation, select a sub-aperture with a small centroid deviation, and complete the wavefront restoration in the form of a reconstructed mode restoration matrix. The method comprehensively considers the non-uniform characteristics of the pupil, and is especially suitable for the Hartmann wavefront detection of pupils with dynamic intensity distribution characteristics. At the same time, it can also provide certain auxiliary functions for the accurate correction of aberrations under the dynamic intensity distribution pupil and the stable decoupling of multiple correctors.
Description
技术领域technical field
本发明属于光学信息测量技术领域,具体涉及一种基于光瞳映射模型的哈特曼波前复原方法。The invention belongs to the technical field of optical information measurement, in particular to a Hartmann wavefront restoration method based on a pupil mapping model.
背景技术Background technique
哈特曼波前传感器是一种兼具高精度和高灵敏度的波前测量手段,已成功应用于自适应光学、光电系统集成、光学检测等领域。哈特曼波前传感器以子孔径阵列的形式,对光学波面进行微分,由子光斑提取子孔径斜率、子波前二阶矩及子孔径光斑反演信息等解算完整波面的相位信息(即,波前信息)。The Hartmann wavefront sensor is a wavefront measurement method with both high precision and high sensitivity, and has been successfully used in adaptive optics, optoelectronic system integration, optical detection and other fields. The Hartmann wavefront sensor differentiates the optical wavefront in the form of a sub-aperture array, and extracts the sub-aperture slope, the second-order moment of the sub-wavefront, and the sub-aperture light spot inversion information from the sub-spot to calculate the phase information of the complete wave front (ie, wavefront information).
当待测光束光瞳强度分布存在空域/时域非均匀特性时,光瞳强度分布对子光斑成像有贡献,可能导致子光斑形态退化甚至缺失,增大波前探测信息的提取误差,影响波前复原结果。因此,针对非均匀强度分布的入射光瞳波前探测,需要发展相应地波前复原手段来提升波前复原精度。近年来已先后发展了“哈特曼波前传感器质心测量精度优化方法”(专利号CN101055223)、“一种采用分时曝光的哈特曼波前传感器”(专利公布号CN102607718A)和“一种适应背景变化点源目标波前探测的夏克-哈特曼波前传感器”(专利公布号CN1971222)等方法,但这些方法均未定量考虑入射光瞳强度分布造成的影响,难以量化波前复原精度优化效果。When the pupil intensity distribution of the beam to be measured has spatial/temporal non-uniformity, the pupil intensity distribution contributes to the sub-spot imaging, which may cause the sub-spot morphology to be degraded or even missing, increase the extraction error of the wavefront detection information, and affect the wavefront Recovery results. Therefore, for the wavefront detection of the entrance pupil with non-uniform intensity distribution, it is necessary to develop corresponding wavefront recovery methods to improve the wavefront recovery accuracy. In recent years, "Hartmann wavefront sensor centroid measurement accuracy optimization method" (patent number CN101055223), "a Hartmann wavefront sensor using time-sharing exposure" (patent publication number CN102607718A) and "a Hartmann wavefront sensor with time-sharing exposure" have been developed successively. However, these methods do not quantitatively consider the influence caused by the intensity distribution of the entrance pupil, and it is difficult to quantify the wavefront recovery. Precision optimization effect.
本发明涉及方法中,针对以上问题,提出基于光瞳映射模型的哈特曼波前复原方法。根据哈特曼波前传感器的入射光瞳信息,通过适当的数据处理方式,提取光瞳分布的时域/空域非均匀性特性导致的子孔径质心偏差,选择质心偏差小的子孔径,通过重构模式复原矩阵的形式完成波前复原。该方法综合考虑了光瞳的非均匀特性,尤其适于具备动态强度分布特性光瞳的哈特曼波前探测。同时,对动态强度分布光瞳下的像差准确校正、多校正器稳定解耦等方面也可提供一定的辅助作用。In the method of the present invention, aiming at the above problems, a Hartmann wavefront restoration method based on the pupil mapping model is proposed. According to the entrance pupil information of the Hartmann wavefront sensor, through appropriate data processing methods, the centroid deviation of the sub-apertures caused by the non-uniformity characteristics of the pupil distribution in time/space domain is extracted, and the sub-aperture with small centroid deviation is selected. The wavefront recovery is completed in the form of a pattern recovery matrix. The method comprehensively considers the non-uniform characteristics of the pupil, and is especially suitable for the Hartmann wavefront detection of pupils with dynamic intensity distribution characteristics. At the same time, it can also provide certain auxiliary functions for the accurate correction of aberrations under the dynamic intensity distribution pupil and the stable decoupling of multiple correctors.
发明内容SUMMARY OF THE INVENTION
本发明要解决的技术问题是:当待测光束光瞳强度分布存在空域/时域非均匀性时,子孔径对应区域的近场光强会影响子光斑形态,造成子孔径波前复原信息的提取误差。针对这一问题,提出一种定量考虑了光瞳强度分布影响的波前复原方法,尽可能减小波前复原误差,提高波前复原精度。The technical problem to be solved by the present invention is: when there is spatial/temporal non-uniformity in the pupil intensity distribution of the beam to be measured, the near-field light intensity in the corresponding area of the sub-aperture will affect the sub-spot shape, resulting in the loss of the sub-aperture wavefront restoration information. Extraction error. Aiming at this problem, this paper proposes a wavefront restoration method that quantitatively considers the influence of pupil intensity distribution, reduces the wavefront restoration error as much as possible, and improves the wavefront restoration accuracy.
本发明要解决其技术问题所采用的技术方案是:一种基于光瞳映射模型的哈特曼波前复原方法,本方法以空域/时域非均匀光瞳下的高精度波前复原为目标,通过入射光瞳强度分析,选择波前复原的有效子孔径,重构模式复原矩阵,完成波前复原。The technical solution adopted by the present invention to solve the technical problem is: a Hartmann wavefront restoration method based on a pupil mapping model, the method aims at high-precision wavefront restoration under the non-uniform pupil in the space/time domain , through the intensity analysis of the entrance pupil, select the effective sub-aperture for wavefront restoration, reconstruct the mode restoration matrix, and complete the wavefront restoration.
具体实现步骤如下:The specific implementation steps are as follows:
步骤(1)、搭建哈特曼波前传感器,在波前探测前获取入射光束的光瞳强度分布信息。光瞳强度分布信息可以随哈特曼波前传感器波前探测过程同步获取,也可以采用光瞳先验信息、预采集或事后处理等形式。Step (1), build a Hartmann wavefront sensor, and obtain the pupil intensity distribution information of the incident beam before wavefront detection. The pupil intensity distribution information can be acquired synchronously with the wavefront detection process of the Hartmann wavefront sensor, or can be obtained in the form of pupil prior information, pre-acquisition or post-processing.
步骤(2)、利用入射光束的光瞳强度分布信息,结合哈特曼波前传感器结构参数,理论计算该光瞳分布在平面波相位下的子光斑图像。分析各子孔径的波前复原信息受光瞳强度分布影响的程度,选择受强度分布影响小的子孔径作为有效子孔径,重构波前复原矩阵;Step (2), using the pupil intensity distribution information of the incident light beam and combining with the structural parameters of the Hartmann wavefront sensor, theoretically calculate the sub-spot image of the pupil distribution under the plane wave phase. Analyze the degree to which the wavefront restoration information of each sub-aperture is affected by the pupil intensity distribution, select the sub-aperture that is less affected by the intensity distribution as the effective sub-aperture, and reconstruct the wavefront restoration matrix;
各子孔径的波前复原信息可以为子孔径斜率,也可以为子波前二阶矩或子孔径光斑反演信息等。The wavefront restoration information of each sub-aperture may be the sub-aperture slope, the second-order moment of the sub-wavefront, or the sub-aperture spot inversion information, or the like.
有效子孔径判据可采用子孔径斜率/二阶矩等信息的理论偏移量或统计值,也可采用子光斑形态分析等方法。The effective sub-aperture criterion may adopt the theoretical offset or statistical value of information such as the sub-aperture slope/second-order moment, and may also adopt methods such as sub-spot morphological analysis.
步骤(3)、将光束入射到哈特曼波前传感器上,采集哈特曼波前传感器的子光斑图像,提取各子孔径波前复原信息,利用重构的波前复原矩阵完成波前复原。各子孔径波前复原信息提取过程中,可并行进一步操作如子孔径减阈值、子孔径加窗、质心修正、斜率加权等。Step (3): Incident the beam on the Hartmann wavefront sensor, collect the sub-spot image of the Hartmann wavefront sensor, extract the wavefront restoration information of each sub-aperture, and use the reconstructed wavefront restoration matrix to complete the wavefront restoration . During the extraction of wavefront restoration information for each sub-aperture, further operations such as sub-aperture subtraction threshold, sub-aperture windowing, centroid correction, and slope weighting can be performed in parallel.
本发明的原理是:通过入射光瞳映射模型获取近场强度分布对哈特曼子光斑影响情况,据此选择哈特曼有效子孔径,利用有效子孔径完成波前复原。The principle of the invention is: obtain the influence of the near-field intensity distribution on the Hartmann sub-spot through the entrance pupil mapping model, select the Hartmann effective sub-aperture accordingly, and use the effective sub-aperture to complete the wavefront restoration.
本发明与现有技术相比具有如下优点:本方法综合考虑了光瞳分布的时间/空间非均匀特性,可望提升非均匀光瞳下哈特曼波前复原的准确性和稳定性。本方法可提高哈特曼波前传感器的实用能力,使异形、闪烁等光瞳条件下的波前准确探测或复原控制成为可能。Compared with the prior art, the present invention has the following advantages: the method comprehensively considers the temporal/spatial non-uniformity of pupil distribution, and is expected to improve the accuracy and stability of Hartmann wavefront restoration under non-uniform pupils. The method can improve the practical ability of the Hartmann wavefront sensor, and make it possible to accurately detect or restore the wavefront under pupil conditions such as irregularities and flickering.
附图说明Description of drawings
图1为本发明的一种基于光瞳映射模型的哈特曼波前复原方法工作光路图,其中,1为分光镜BS,2为微透镜阵列,3为哈特曼探测器,4为光瞳探测器;1 is a working light path diagram of a Hartmann wavefront restoration method based on pupil mapping model of the present invention, wherein 1 is a spectroscope BS, 2 is a microlens array, 3 is a Hartmann detector, and 4 is a light pupil detector;
图2为本发明涉及方法与传统方法对空域非均匀近场的波前复原结果对比图;FIG. 2 is a comparison diagram of the wavefront restoration results of the method involved in the present invention and the traditional method for the non-uniform near-field in the spatial domain;
图3为本发明的一种基于光瞳映射模型的哈特曼波前复原方法的工作流程图。FIG. 3 is a working flow chart of a Hartmann wavefront restoration method based on a pupil mapping model of the present invention.
具体实施方式Detailed ways
下面结合附图以及具体实施方式进一步说明本发明。The present invention will be further described below with reference to the accompanying drawings and specific embodiments.
如图2所示,本发明的一种基于光瞳映射模型的哈特曼波前复原方法的具体实施方式如下:As shown in Figure 2, the specific embodiment of a Hartmann wavefront restoration method based on a pupil mapping model of the present invention is as follows:
步骤(1)、搭建哈特曼波前传感器,同步采集光瞳强度分布图像。本实施例中,哈特曼波前传感器子孔径共76个,正方形布局,每个子孔径尺寸1mm×1mm,焦距21.7mm。入射光瞳Φ10mm,强度动态非均匀,光强填充因子F在0.2~0.8之间(F因子越低,表示近场光强越不均匀)。拟探测前15阶泽尼克模式像差。Step (1), build a Hartmann wavefront sensor, and collect pupil intensity distribution images synchronously. In this embodiment, the Hartmann wavefront sensor has a total of 76 sub-apertures in a square layout, each sub-aperture has a size of 1 mm×1 mm, and a focal length of 21.7 mm. The entrance pupil is Φ10mm, the intensity is dynamically non-uniform, and the light intensity filling factor F is between 0.2 and 0.8 (the lower the F factor, the more non-uniform the near-field light intensity is). It is intended to detect the first 15th order Zernike mode aberrations.
如图1所示,哈特曼波前传感器包括微透镜阵列2和哈特曼探测器3。待测光束经分光镜BS 1分光,一部分经微透镜阵列2聚焦成像在哈特曼探测器3上,另一部分入射到光瞳探测器4。光瞳探测器4用来获得光瞳映射模型,哈特曼探测器3根据成像光斑阵列和光瞳映射模型进行波前复原。As shown in FIG. 1 , the Hartmann wavefront sensor includes a
步骤(2)、利用入射光束的光瞳强度分布信息,结合哈特曼波前传感器结构参数,理论计算该光瞳分布在平面波相位下的子光斑图像。分析各子孔径斜率受光瞳强度分布影响的程度,选择受强度分布影响小的子孔径作为有效子孔径,重构波前复原矩阵;Step (2), using the pupil intensity distribution information of the incident light beam and combining with the structural parameters of the Hartmann wavefront sensor, theoretically calculate the sub-spot image of the pupil distribution under the plane wave phase. Analyze the degree to which the slope of each sub-aperture is affected by the pupil intensity distribution, select the sub-aperture that is less affected by the intensity distribution as the effective sub-aperture, and reconstruct the wavefront restoration matrix;
本实施例中,哈特曼波前传感器提取各子孔径斜率的同时,根据光瞳强度分布计算各子孔径在近场影响下斜率偏移情况,选择斜率偏离0.1像素的子孔径为有效子孔径。根据有效子孔径序号重构模式复原矩阵。In this embodiment, while extracting the slope of each sub-aperture, the Hartmann wavefront sensor calculates the slope shift of each sub-aperture under the influence of the near field according to the pupil intensity distribution, and selects the sub-aperture whose slope deviates from 0.1 pixel as the effective sub-aperture . The mode restoration matrix is reconstructed according to the effective sub-aperture number.
哈特曼探测器得到的光斑阵列斜率信息记为S,根据光瞳映射模型得到的斜率误差矩阵为Se。S和Se为相同维度的矩阵。若abs(Se)>0.1,则对应序号的斜率S置零,并认为是无效子孔径。然后根据有效子孔径序号重构模式复原矩阵G。The slope information of the light spot array obtained by the Hartmann detector is denoted as S, and the slope error matrix obtained according to the pupil mapping model is Se. S and Se are matrices of the same dimension. If abs(Se)>0.1, the slope S of the corresponding serial number is set to zero, and it is considered to be an invalid sub-aperture. Then, the mode restoration matrix G is reconstructed according to the effective sub-aperture number.
步骤(3)、利用重构的波前复原矩阵完成波前复原。具体计算过程为:复原波前W=GS。Step (3), using the reconstructed wavefront restoration matrix to complete the wavefront restoration. The specific calculation process is as follows: the restoration wavefront W=GS.
在本实施例中,统计了6000组不同近场分布在一定像差水平下的波前复原结果。光场近场填充因子在0.2~0.8之间波动,平均F≈0.5,输入波前RMS≈2λ。统计表明,本哈特曼波前传感器在均匀近场下,波前复原残差RMS≈0.18λ;而非均匀近场下,本方法和传统方法的复原残差如图2所示,可以看出,通过选择有效子孔径,可以提高波前复原精度,在F因子较低时,优化效果更为明显。统计结果中,F≤0.4的数据约1800组,传统方法平均复原残差RMS≈0.50λ,本方法平均复原残差RMS≈0.38λ。若配合斜率修正等措施,波前复原精度有望进一步提升。In this embodiment, 6000 groups of wavefront restoration results of different near-field distributions under a certain aberration level are counted. The near-field fill factor of the optical field fluctuates between 0.2 and 0.8, with an average F≈0.5, and the input wavefront RMS≈2λ. Statistics show that the wavefront restoration residual RMS ≈ 0.18λ of the Ben Hartmann wavefront sensor in the uniform near field; under the non-uniform near field, the restoration residuals of this method and the traditional method are shown in Figure 2. It can be seen that It can be seen that by selecting the effective sub-aperture, the wavefront restoration accuracy can be improved, and the optimization effect is more obvious when the F factor is low. In the statistical results, there are about 1800 groups of data with F≤0.4, the traditional method has an average restoration residual RMS≈0.50λ, and this method has an average restoration residual RMS≈0.38λ. If combined with slope correction and other measures, the wavefront restoration accuracy is expected to be further improved.
本发明说明书中未作详细描述的内容属于本领域专业技术人员公知的现有技术。Contents that are not described in detail in the specification of the present invention belong to the prior art known to those skilled in the art.
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