Very low noise Shack-Hartmann wavefront sensor for adaptive optics in the near-IR

2014 ◽  
Author(s):  
Silvère Gousset ◽  
Clélia Robert ◽  
Thierry Fusco ◽  
Vincent Michau ◽  
Cyril Petit ◽  
...  
1994 ◽  
Vol 158 ◽  
pp. 308-310
Author(s):  
David W. Tyler ◽  
Gary C. Loos

Two high-fidelity computer simulations are used to study low-order adaptive optics systems operating in the near-infrared. We study obtainable system performance using very dim reference sources at three IR wavelengths.


2014 ◽  
Author(s):  
Jean-Luc Gach ◽  
Philippe Feautrier ◽  
Philippe Balard ◽  
Christian Guillaume ◽  
Eric Stadler

2006 ◽  
Author(s):  
Matthew A. Kenworthy ◽  
Philip M. Hinz ◽  
Suresh Sivanandam ◽  
Andrew H. Breuninger ◽  
Frank J. Low

2009 ◽  
Vol 17 (22) ◽  
pp. 20575 ◽  
Author(s):  
Zhiwen Wu ◽  
Anita Enmark ◽  
Mette Owner-Petersen ◽  
Torben Andersen

2020 ◽  
Vol 636 ◽  
pp. A88 ◽  
Author(s):  
S. Esposito ◽  
A. Puglisi ◽  
E. Pinna ◽  
G. Agapito ◽  
F. Quirós-Pacheco ◽  
...  

The paper deals with with the on-sky performance of the pyramid wavefront sensor-based Adaptive Optics (AO) systems. These wavefront sensors are of great importance, being used in all first light AO systems of the ELTs (E-ELT, GMT, and TMT), currently in design phase. In particular, non-common path aberrations (NCPAs) are a critical issue encountered when using an AO system to produce corrected images in an associated astronomical instrument. The AO wavefront sensor (WFS) and the supported scientific instrument typically use a series of different optical elements, thus experiencing different aberrations. The usual way to correct for such NCPAs is to introduce a static offset in the WFS signals. In this way, when the AO loop is closed the sensor offsets are zeroed and the deformable mirror converges to the shape required to null the NCPA. The method assumes that the WFS operation is linear and completely described by some pre-calibrated interaction matrix. This is not the case for some frequently used wavefront sensors like the Pyramid sensor or a quad-cell Shack-Hartmann sensor. Here we present a method to work in closed-loop with a pyramid wavefront sensor, or more generally a non-linear WFS, introducing a wavefront offset that remains stable when AO correction quality changes due to variations in external conditions like star brightness, seeing, and wind speed. The paper details the methods with analytical and numerical considerations. Then we present results of tests executed at the LBT telescope, in daytime and on sky, using the FLAO system and LUCI2 facility instrument. The on-sky results clearly show the successful operation of the method that completely nulls NCPA, recovering diffraction-limited images with about 70% Strehl ratio in H band in variable seeing conditions. The proposed method is suitable for application to the above-mentioned ELT AO systems.


1998 ◽  
Author(s):  
Armando Riccardi ◽  
N. Bindi ◽  
Roberto Ragazzoni ◽  
Simone Esposito ◽  
Paolo Stefanini

2006 ◽  
Vol 23 (20) ◽  
pp. 5919-5925
Author(s):  
S Avino ◽  
E Calloni ◽  
A Tierno ◽  
B Agrawal ◽  
R De Rosa ◽  
...  

2007 ◽  
Vol 3 (S248) ◽  
pp. 106-107
Author(s):  
M. Gai ◽  
D. F. Buscher ◽  
L. Corcione ◽  
S. Ligori ◽  
J. S. Young

AbstractInterferometry in the near IR aims at providing imaging resolution on the mas scale, and astrometry at the few μas level, from ground based infrastructures using current telescope technology. To take advantage of simultaneous combination of four to eight telescopes, an international consortium is proposing to ESO the development of the VLTI Spectro-Imager. One of the key sub-systems, to measure and correct the atmospheric perturbations relative to the beam phase, is the fringe tracker, aimed at providing the science combiner with long, stable observing conditions. The fringe tracker function in interferometer is equivalent to adaptive optics for conventional telescopes. The fringe tracker concept under study, using minimum redundancy combination and bulk optics, is described.


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