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High Contrast Imaging with Focal Plane Wavefront Sensing and PIAA for Subaru Telescopes Olivier Guyon Basile Gallet

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Presentation on theme: "High Contrast Imaging with Focal Plane Wavefront Sensing and PIAA for Subaru Telescopes Olivier Guyon Basile Gallet"— Presentation transcript:

1 High Contrast Imaging with Focal Plane Wavefront Sensing and PIAA for Subaru Telescopes Olivier Guyon (guyon@naoj.org) Basile Gallet (gallet@naoj.org) Eugene Pluzhnik (pea@naoj.org)pea@naoj.org Hideki Takami (takami@naoj.org)takami@naoj.org Shinichiro Takana Subaru Telescope / National Astronomical Observatory of Japan Motohide Tamura Lyu Abe National Astronomical Observatory of Japan Subaru AO team & HiCIAO team

2 Introduction / Outline Goal: high contrast at low inner working angle (IWA) Half the IWA = 8x more accessible planets 0.1'' – 0.2'' has 7x more planets than >0.2'' lots of science possible with ~1k actuators Reflected light from closeby planets is stronger at ~0.1''-0.2'', 1e8 contrast for some RV planets

3 High-contrast AO at Subaru Telescope AO188 188 elements curvature system (first light: end 2006) HiCIAO differential imaging near-IR camera (2007) ''Tweeter'' + low IWA coronagraph Nasmyth focus flexible & friendly environment PIAA

4 PIAA / APLC Hybrid coronagraph Angular separation Useful Throughput

5 Why focal plane wavefront sensing ? ''What you see is exactly what you want to remove'' Main sources of wavefront errors : - Photon noise - Time lag - Fitting errors # of elements Aliasing - Non-common path errors optical components (static) actuator vs. WFS registration (static & dynamic) - scintillation - wavefront chromaticity refraction index of air (OPD chromaticity) Fresnel propagation (OPD and ampl. Chromaticity) chromatic shear of wavefront

6 ''fundamental'' contrast limitations of AO with vis. WFS & near-IR imaging 8m telesc. V WFS H imaging (Guyon, 2005)

7 Wavefront sensors ''efficiencies'' (Guyon 2005) Square root of # of photons required to reach fixed sensing accuracy plotted here for phase aberrations only.

8 ''Dark Hole'' DM control If wavefront is known, DM can be controlled to ''perfectly'' cancel speckles JPL High contrast imaging testbed Malbet, Yu & Shao (1995) Guyon (2005) Give'on (2003-2006) Borde & Traub (2006)

9 Fast(er) algorithm using linear approximations – few ms on single CPU, code not optimized for speed

10 PIAA coronagraph development at Subaru co-funded by JPL and Subaru/NAOJ Utilizes lossless beam apodization with aspheric optics (mirrors or lenses) to concentrate starlight is single diffraction peak (no Airy rings). - high contrast - Nearly 100% throughput - IWA < 2 l/d - 100% search area - no loss in angular resol. - can remove central obsc. and spiders - achromatic (with mirrors) For Subaru, Lyot Coronagraph with PIAA- apodized input pupil. IWA ~ 1 lambda/d

11 Early demonstration in lab (Galicher et al. 2005) Lenses made by Masashi Otsubo (ATC, NAOJ)

12 PIAA mirror units (Axsys) JPL-funded TPF-C technology development

13 32x32 MEMs DM is used for FPAO test in lab with PIAA coronagraph One of 14 boards to drive the MEMs DM. 80 channels/board 16 bit resolution slow & fast interface (> kHz update) S. Colley AO electronic eng. Subaru Telescope

14 Closed loop WFC Without prior knowledge, 3 frames sufficient for WF measurement

15 Low Order Wavefront Sensor (LOWFS) LOWFS performance Small (<<lambda) wavefront error produces large flux changes in the LOWFS images


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