The presence of 51-cm wide spiders supporting the secondary mirror of the Extremely Large Telescope breaks the wave-front continuity of the incoming light and suggests to consider the telescope pupil as 6 independent petals, each of them having a di erent piston value. It is therefore necessary to co-phase them in order to return to a single continuous wave-front. Not being corrected, these phase steps in the pupil would severely decrease the optical performance. As part of MICADO instrument Single Conjugate Adaptive Optics (SCAO), a Pyramid wave-front Sensor (P-WFS) is being used to provide a measurement of the aberrated wave-front. Di ractive optics enables to describe phase steps accross the pupil as a signal in the wave-front sensor focal plane: a piston applied on one of the 6 segments will create a speci c pattern on the detector plane of the P-WFS so that it should in principle be possible to detect it. However, in practice, the sensor is not sensitive enough to di erential piston due to other wave-front errors and it drives M4 to take unintended piston values on its six segments. This e ect is known as petalling. The adaptive optics end-to-end simulation platform COMPASS allows to perform numerical simulations in closed loop and quantify the impact of IE on the SCAO performance. Speci cally, we investigate the P-WFS di erential piston sensing capability under atmospheric turbulence, with remaining closed-loop residuals. We show that these residuals are read as spurious di erential piston : this error being additive throughout the time, the di erential piston varies rapidly and reaches values up to a few microns. To cope with this e ect, we set up a minimum mean-square error (MMSE) reconstructor dedicated to di erential piston estimation control and we compare the results with the already implemented slaved actuators method.
[1]
S. Esposito,et al.
Pyramid Wavefront Sensor behavior in partial correction Adaptive Optic systems
,
2001
.
[2]
S Esposito,et al.
Signal spatial filtering for co-phasing in seeing-limited conditions.
,
2007,
Optics letters.
[3]
A. Sevin,et al.
Real-time end-to-end AO simulations at ELT scale on multiple GPUs with the COMPASS platform
,
2018,
Astronomical Telescopes + Instrumentation.
[4]
Fabrice Vidal,et al.
End-to-End simulations for the MICADO-MAORY SCAO mode
,
2017
.
[5]
Pierre Baudoz,et al.
The MICADO first-light imager for the ELT: towards the preliminary design review of the MICADO-MAORY SCAO
,
2018,
Astronomical Telescopes + Instrumentation.
[6]
Nicholas Devaney,et al.
Segmented telescopes co-phasing using Pyramid Sensor
,
2002
.
[7]
R. Ragazzoni,et al.
Sensitivity of a pyramidic Wave Front sensor in closed loop Adaptive Optics
,
1999
.
[8]
Jean-Franccois Sauvage,et al.
Sensing and control of segmented mirrors with a pyramid wavefront sensor in the presence of spiders
,
2017
.
[9]
R. Ragazzoni.
Pupil plane wavefront sensing with an oscillating prism
,
1996
.
[10]
Richard M. Myers,et al.
Phase ambiguity solution with the Pyramid Phasing Sensor
,
2006,
SPIE Astronomical Telescopes + Instrumentation.
[11]
Christopher Dainty,et al.
Linearity of the pyramid wavefront sensor.
,
2006,
Optics express.
[12]
G. Rousset,et al.
A telescope-ready approach for modal compensation of pyramid wavefront sensor optical gain
,
2019,
Astronomy & Astrophysics.
[13]
Armando Riccardi,et al.
Laboratory test of a pyramid wavefront sensor
,
2000,
Astronomical Telescopes and Instrumentation.