Chinese Optics, Volume. 15, Issue 5, 992(2022)
Detection of large aperture flat mirror based on the differential optics transfer function method
Fig. 1. Principal component analysis results of standard wavefront
Fig. 2. (a) The amplitude and (b) phase calculated by the differential optical transfer function for the mixed wavefront of coma and astigmatism
Fig. 3. Energy distributions of the focal spot before (a) and after (b) aperture variation
Fig. 4. Differential optical transfer function solutions for a 2 m level large aperture mirror shape. (a) Original wavefront. (b) Recovered wavefront. (c) Original wavefront structure function. (d) Recovered wavefront structure function
Fig. 5. Cross correlation function between the original wavefront and restoration′s result
Fig. 6. Large aperture planar mirror discrete aperture detection architecture based on holographic Ritchey-Common detection. (a) Pupil architecture. (b) Detection optical path. (c) Aperture variational calculation process
Fig. 7. (a) Original wavefront and (b) reconstructed wavefront of low-order aberration combination
Fig. 8. Comparison of Zernike coefficients corresponding to the original wavefront and the reconstructed wavefront
Fig. 9. (a) The amplitude and (b) phase information obtained from the solution and (c) the implementation device
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Qi-chang AN, Xi-wen JIANG, Hong-wen LI, Jing TANG. Detection of large aperture flat mirror based on the differential optics transfer function method[J]. Chinese Optics, 2022, 15(5): 992
Category: Original Article
Received: Jun. 13, 2022
Accepted: --
Published Online: Sep. 29, 2022
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