Analysis and mitigation of pupil discontinuities on adaptive optics performance

As already noticed in other telescopes, the presence of large telescope spiders and of a segmented deformable mirror in an Adaptive Optics system leads to pupil fragmentation and may create phase discontinuities. On the ELT telescope, a typical effect is the differential piston, where all disconnected areas of the pupil create their own piston, unseen locally but drastically degrading the final image quality. The poor sensitivity of the Pyramid WFS to differential piston will lead to these modes been badly seen and therefore badly controlled by the adaptive optics (AO) loop. In close loop operation, differential pistons between segments will start to appear and settle around integer values of the average sensing wavelength. These additional differential pistons are artificially injected by the adaptive optics control loop but do not have any real physical origin, contrary to the Low Wind Effect. In an attempt to reduce the impact of unwanted differential pistons that are injected by the AO loop, we propose a novel approach based on the pair-wise coupling of the actuators sitting on the edges of the deformable mirror segments. In this paper, we present the correction principle, its performance in nominal seeing condition, and its robustness relative to changing seeing conditions, wind speed and natural guide star magnitude. We show that the edge actuator coupling is a simple and robust solution and that the additional quadratic error relative to the reference case (i.e. no spiders) is of only 40 nm RMS, well within the requirements for HARMONI.

[1]  Kjetil Dohlen,et al.  HARMONI at the diffraction limit: from single conjugate to laser tomography adaptive optics (Conference Presentation) , 2018, Adaptive Optics Systems VI.

[2]  Michel Tallon,et al.  Adaptive Optics for Extremely Large Telescopes III Of Spiders and elongated spots , 2013 .

[3]  Jean-Franccois Sauvage,et al.  Sensing and control of segmented mirrors with a pyramid wavefront sensor in the presence of spiders , 2017 .

[4]  T. Fusco,et al.  The adaptive optics modes for HARMONI: from Classical to Laser Assisted Tomographic AO , 2016, Astronomical Telescopes + Instrumentation.

[5]  Frantz Martinache,et al.  Calibration of the island effect: Experimental validation of closed-loop focal plane wavefront control on Subaru/SCExAO , 2017 .

[6]  Kjetil Dohlen,et al.  Tackling down the low wind effect on SPHERE instrument , 2016, Astronomical Telescopes + Instrumentation.

[7]  Kjetil Dohlen,et al.  Preparation of AO-related observations and post-processing recipes for E-ELT HARMONI-SCAO , 2016, Astronomical Telescopes + Instrumentation.

[8]  T. Fusco,et al.  A "Fast and Furious'" solution to the low-wind effect for SPHERE at the VLT , 2016, Astronomical Telescopes + Instrumentation.

[9]  Fernando Quirós-Pacheco,et al.  Performance of the Giant Magellan Telescope phasing system , 2016, Astronomical Telescopes + Instrumentation.

[10]  Pierre-Yves Madec,et al.  Wavefront reconstruction with pupil fragmentation: study of a simple case , 2016, Astronomical Telescopes + Instrumentation.

[11]  T. Fusco,et al.  Low wind effect on VLT/SPHERE: impact, mitigation strategy, and results , 2018, Astronomical Telescopes + Instrumentation.

[12]  Johan Kosmalski,et al.  The E-ELT first light spectrograph HARMONI: capabilities and modes , 2016, Astronomical Telescopes + Instrumentation.

[13]  S. Esposito,et al.  Pyramid sensor for segmented mirror alignment. , 2005, Optics letters.

[14]  Thierry Fusco,et al.  Iterative wave-front reconstruction in the Fourier domain. , 2017, Optics express.

[15]  C Verinaud,et al.  Adaptive-optics correction of a stellar interferometer with a single pyramid wave-front sensor. , 2002, Optics letters.