2001
DOI: 10.1051/0004-6361:20000185
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Piston control with adaptive optics in stellar interferometry

Abstract: Abstract. The general purpose of an adaptive optics system is to correct for the wavefront corrugations due to atmospheric turbulence. When applied to a stellar interferometer, care must be taken in the control of the mean optical path length, commonly called differential piston. This paper defines a general formalism for the piston control of a deformable mirror in the linear regime. It is shown that the usual filtering of the piston mode in the command space is not sufficient, mostly in the case of a bimorph… Show more

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Cited by 14 publications
(7 citation statements)
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References 16 publications
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“…-Bimorph piston effect: this is the OPD induced by resonances of the adaptive optics deformable mirror (Vérinaud & Cassaing 2001). This contribution has been evaluated for the MACAO adaptive optics at VLTI, and turns out to be dominant above 100 Hz despite the use of a "piston-free" algorithm for the control of the deformable mirror.…”
Section: The Piston Effectmentioning
confidence: 99%
“…-Bimorph piston effect: this is the OPD induced by resonances of the adaptive optics deformable mirror (Vérinaud & Cassaing 2001). This contribution has been evaluated for the MACAO adaptive optics at VLTI, and turns out to be dominant above 100 Hz despite the use of a "piston-free" algorithm for the control of the deformable mirror.…”
Section: The Piston Effectmentioning
confidence: 99%
“…Such effect would reduce the fringe contrast at the recombination laboratory and be detrimental to the performance of the Interferometer. The piston mode removal algorithm implemented had been first described in 6 . Most of the piston characterization & tune-up takes place in the laboratory where a setup has been designed in order to do so.…”
Section: Piston Performancementioning
confidence: 99%
“…where A and B are constants and Φ i (ν) is chosen randomly for each sampled temporal frequency ν. For Kolmogorov turbulence, the fast scan ( 1 s) regime has B = 17/6 (Conan et al 1995) but there is experimental evidence (di Folco et al 2003) that the slope is not as steep at VLTI, with simulations by Absil et al (2006) explaining it in terms of the piston induced at high frequency by the adaptive optics (imperfect) correction ("bimorph piston", see Vérinaud & Cassaing 2001) and wavefront errors produced by the injection into single-mode waveguides ("coupled piston", see Ruilier & Cassaing 2001). Linfield et al (1999) have also measured a deviation from the Kolmogorov behaviour at PTI.…”
Section: Numerical Modellingmentioning
confidence: 99%