Abstract

The performance of the “weighted Fourier phase slope” centroiding algorithm at the subpupil image of a Shack–Hartmann wavefront sensor for point-like astronomical guiding sources is explored. This algorithm estimates the image’s displacement in the Fourier domain by directly computing the phase slope at several spatial frequencies, without the intermediate step of computing the phase; it then applies optimized weights to the phase slopes at each spatial frequency obtained by a Bayesian estimation method. The idea was inspired by cepstrum deconvolution techniques, and this relationship is illustrated. The algorithm’s tilt estimation performance is characterized and contrasted with other known centroiding algorithms, such as thresholded centre of gravity (TCoG) and cross correlation (CC), first through numerical simulations at the subpupil level, then at the pupil level, and finally at the laboratory test bench. Results show a similar sensitivity to that of the CC algorithm, which is superior to that of the TCoG algorithm when large fields of view are necessary, i.e., in an open-loop configured adaptive optics system, thereby increasing the guide star limiting magnitude by 0.6 to 0.7 mag. On the other side, its advantage over the CC algorithm is its lower computational cost by approximately an order of magnitude.

Highlights

  • The Shack–Hartmann wavefront sensor (SHWFS) continues to be the most widely used wavefront sensor in astronomy with the most mature technology

  • We present the characterization and comparative performance results of a centroiding method formulated as an optimized Bayesian estimator in the Fourier domain, for Shack–Hartmann wavefront sensors and point-like guiding sources, which we have called the weighted Fourier phase slope (WFPS) algorithm

  • For light levels from below 20 to beyond 200 photons per subaperture, both cross correlation (CC) and WFPS algorithms outperform the thresholded centre of gravity (TCoG) method owing to their capacity to neutralize detector noise, and this improvement becomes more evident for increasing field of view (FoV)

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Summary

Introduction

The Shack–Hartmann wavefront sensor (SHWFS) continues to be the most widely used wavefront sensor in astronomy with the most mature technology. The estimation of such displacements allows to retrieve the aberrated incident wavefront profile.[1] This sensor’s parameters, such as the pupil’s sampling factor and subpupil’s image field of view (FoV) and resolution, can be selected according to the application requirements of wavefront estimation precision, sensitivity, and dynamic range This flexibility is in contrast to other wavefront sensing techniques, for example, the pyramid wavefront sensor (P-WFS).[2] This other technique achieves greater sensitivity than the SHWFS but relies for its operation on the at least partial correction of the wavefront aberration to reduce its dynamic range.[3].

Description of the Weighted Fourier Phase Slope Algorithm
Description of the Simulator
Optimum Field of View
Maximum-a-Posteriori Weights
Sensitivity Performance
Performance Simulations at Pupil Level
Laboratory Test
Findings
Conclusions and Future Work
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