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The successful detection of gravitational waves not only validate the general theory of relativity but also unveile previously undetectable cosmic events, opening new research directions for both physics and astronomy. Laser interferometers, characterized by their high sensitivity and broad frequency response, have become the primary method for gravitational wave detection. Due to the constraints imposed by terrestrial conditions, the frequency range for ground-based detection is quite limited, necessitating the exploration of space-based gravitational wave detection. Within this space-based detection framework, spaceborne telescopes serve as the core component. These telescopes require robust capabilities for interferometric laser transmission and reception, as well as high-precision tracking to accurately measure and detect gravitational wave events. Throughout their operation, these telescopes are affected by temperature variations in space, mechanical stresses or vibrations caused by launches or other space operations, thermal effects or expansions, and, over time, aging, degradation, or minor structural changes in the materials and components, all of which can result in wavefront aberrations. Such aberrations can directly influence the energy distribution and spatial position of the far-field light spot after being transmitted over hundreds of thousands of kilometers, subsequently limiting the interference quality and, in turn, the gravitational wave detection capability. To minimize the impact of wavefront aberrations on space-based gravitational wave detection, this paper introduces a frequency domain covariance algorithm for noise thresholding, replacing the threshold centroid algorithm for offset position estimation, and enhancing detection precision by incorporating multi-aperture multiplexing technology. By applying the frequency domain covariance algorithm and the threshold centroid algorithm to the slope measurement and wavefront reconstruction of actual point source images with added defocus values, we concluded that the former achieves higher measurement accuracy than the latter. The calculated defocus value and root mean square (RMS) of the residual wavefront further verified the computational precision of the relevant algorithms and their superior performance over the centroid algorithm. In comparison to the threshold centroid method, our approach exhibits greater accuracy in wavefront aberration measurement, achieving a precision of up to λ/3000. This study not only deepens our understanding of wavefront aberrations in gravitational wave detection but also paves the way for enhancing the precision and accuracy of gravitational wave detection.
Optical layout design of the spaceborne telescope for TianQin Project
The principle of the Shack-Hartmann wavefront sensor
Image matching principle of correlation algorithm
The optical path diagram of the experimental platform
Effective sub-aperture distribution of the point source image
Individual sub-aperture image and noise calculation region (within the yellow box) and matching region (within the red box)
The average shift measured on each frame image by employing the CFF and the TCoG algorithm. Defocus values are (a) 0 nm, (b) 0.22 nm, (c) 0.44 nm and (d) 0.66 nm
Zernike defocus values, and their average calculated on each frame image by employing the CFF and the TCoG algorithm. Defocus values are (a) 0 nm, (b) 0.22 nm, (c) 0.44 nm and (d) 0.66 nm
The average reconstructed wavefront using the CFF and the TCoG algorithm. Defocus values are (a) 0 nm, (b) 0.22 nm, (c) 0.44 nm and (d) 0.66 nm
The residual wavefront generated using the CFF and the TCoG algorithm. Defocus values are (a) 0 nm, (b) 0.22 nm, (c) 0.44 nm and (d) 0.66 nm
The process of wavefront reconstruction and the composition of reconstruction error