Adaptive optics for SOAR
Andrei Tokovinin (CTIO)
More information:
http://www.ctio.noao.edu/~atokovin/soar/
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Do we need AO?
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What can and can not be done with AO?
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System concept and performance
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Preliminary plan
SOAR niche
Science case for AO at SOAR
The case for high angular resolution is evident!
See images with 0.3" and 0.7" resolution.
Improved seeing in a large (3') FOV
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Rival 8 m telescopes in background-limited sensitivity
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Best ground-based sensitivity in crowded fields
Diffraction limit, small (10") FOV
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Optical: UNIQUE capability, 0.03" resolution
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IR: lose to Gemini 2 times in resolution, 4 times in sensitivity, 16 times
in exposure time to reach given S/N.
Seeing at Cerro Pachon
Source: Gemini RPT-AO-G0094
Revised seeing
r0 at zenith at 0.5 micron |
- Median: 15 cm (FWHM 0.67")
- Good (25%): 20 cm (FWHM 0.50")
- 75%: 10.7 cm (FWHM 0.94")
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Finite turbulence outer scale ~25 m
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- Less tip-tilt (compared to standard theory)
- Better uncompensated seeing
- More improvement in the IR
- Less improvement from tip-tilt
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Revised "isokinetic patch"
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4 m/ 16 km = 51"
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Mean turbulence profile at Cerro Pachon (1998, 22 nights).
Seeing improvement with AO
Improve wave-front coherence at r0 scale .
Idea 1: Low-order compensation =
incoherent combination of 1 m
sub-apertures. Example: CFHT+PUEO. Gain in FWHM: ~2 times. Small FOV.
Idea 2: Compensate only low layers.
Gain in FWHM: ~2 times. Large FOV.
- Several NGSs and tomography (but: not enough photons)
- Rayleigh LGS: good, insensitive to high layers!
PSFs under good seeing at 0.67 micron: Full line: uncompensated (leftmost)
and with tip-tilt.
Dashed line: AO+LGS at 10 km.
Diffraction-limited AO
Improve wave-front coherence across full aperture.
- Need NGS -> small sky coverage (but: LMC, Galactic plane!)
- Small compensated FOV
PSFs under good seeing at 0.67 micron with 12m NGS. The leftmost
PSF is for uncompensated image under same conditions.
Limiting magnitude?
Strehl ratio on-axis and at 4" off-axis versus NGS R-magnitude. Good seeing,
0.67 micron.
PUEO: 1-m sub-apertures -> 15m
SOAR: 0.5-m sub-apertures -> 13m?
Comparing tip-tilt, seeing improvement
and full AO
- Compensation changes the PSF structure: becomes more peaked
- Maximum gain in Strehl and FWHM
- Lower gain in encircled energy and detectivity
Performance: FWHM
FWHM on-axis, median seeing
Good match between seeing-improved resolution in the visible and
seeing limit in the IR.
FWHM on-axis, good seeing
Performance: Central intensity = Strehl
Performance: Encircled energy
System concept
- Small (~1 m size) AO module on the optical ISB
- DM: OKO Tech, 35 mm beam diameter, 70-120 actuators
- WFS: Shack-Hartmann, curvature or pyramid (TBD)
- LGS: Rayleigh, solid-state UV laser, 10-20 km altitude
- TTS: three sensors, to be used with LGS
- Three scientific instruments, switchable
- Imager: 2K CCD, red-optimized, pixels 100 and 15 mas
- IFU spectrometer: 2 plate scales
- Third instrument: TBD, reserved for future
Implementation plan
RESOURCES:
2002 - NOAO internal (design study)
2003-2005: NOAO+SOAR? $500K?
Summary: We want to design a USEFUL system which combines unique
high-resolution capability in the optical with seeing improvement
mode.
It must be cheap!