Abstract

To achieve a full-aperture, diffraction-limited image, a telescope’s segmented primary mirror must be properly phased. Furthermore, it is crucial to detect the piston errors between individual segments with high accuracy. Based on the diffraction imaging theory, the symmetrically shaped aperture with an arbitrarily positioned entrance pupil would focus at the optical axis with a symmetrical diffraction pattern. By selecting a single mirror as a reference mirror and regarding the diffraction image’s center as the calibration point, a function can be derived that expresses the relationship between the piston error and the distance from the center of the inference image to the calibration point is linearity within one-half wavelength. These theoretical results are shown to be consistent with the results of a numerical simulation. Using this method, not only the piston error, but also the tip–tilt error can be detected. This method is simple and effective; it yields high-accuracy measurements and requires less computation time.

Highlights

  • The segmented primary mirror is one of the best choices for constructing a large telescope

  • From Eqs. (3) and (5), we see that if tip–tilt error exists in the phase function, the center of the diffraction image of the aperture deviates from the ideal optical axis

  • We conclude that the rectangular aperture with an arbitrarily positioned entrance pupil will image at the optical axis of the testing system with a symmetric diffraction shape

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Summary

Introduction

The segmented primary mirror is one of the best choices for constructing a large telescope. The world’s largest telescopes—e.g., Keck, HET, LAMOST, TMT—all adopt segmented primary mirrors. Numerical simulations are carried out, and the results are shown to be consistent with the theoretical calculation results. This detection method is simple, efficient, and highly accurate. We analyze the interference image of two adjacent rectangular apertures with piston error, and deduce the relation between the piston error (between two adjacent segmented mirrors) and the position of the center of the interference image. Numerical simulations are carried out in order to verify the theoretical equations

Theory
Calculating the Center of the Diffraction Image
Example of Numerical Simulation
Conclusions
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