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TMT Construction Proposal - Thirty Meter Telescope

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To the extent consistent with these shielding requirements, the enclosure should allow natural air venting of the<br />

primary mirror to reduce M1 seeing.<br />

To minimize thermal differences that will degrade image quality, the enclosure interior should be cooled during<br />

the day so the telescope is at the expected night-time temperature.<br />

3.5 Adaptive Optics<br />

Diffraction-limited observations are a key capability of <strong>TMT</strong>, and this will be delivered by the AO system. Ideally<br />

we would like to make diffraction-limited observations over the entire sky and for all wavelengths. Our<br />

understanding of the technology suggests this will not be available in the foreseeable future, so we have made<br />

some compromises in the required early AO capability.<br />

We will eventually want an AO system that can deliver rms wavefront errors of ~ 130 nm with full sky coverage,<br />

corresponding to a Strehl ratio of 0.5 at 1µm. For a range of cost, schedule, and technical considerations, we<br />

will accept a first-light AO capability with 187-191 nm rms wavefront error over a 10 arcsec field of view. This<br />

corresponds to a Strehl of 0.5 at 1.36µm. The AO system must deliver this performance over a majority of the<br />

sky (e.g. 50% sky coverage at the galactic pole). This sky coverage is expected to be achieved with a multiple<br />

laser beacon system. A subsequent upgrade will reduce the AO system noise to 130 nm.<br />

We anticipate several valuable modes of AO:<br />

Narrow-Field, Diffraction-limited, Near IR, or narrow Field IR Adaptive Optics System (NFIRAOS) will be used<br />

for NIR spectroscopy and can feed an on-axis integral field unit (IFU) and sample the image at the diffraction<br />

limit. A small field is sufficient (10 arcsec) as long as we have close to 50% sky coverage. Image motion will<br />

degrade image size over a higher fraction of the sky. Again, we expect that a Laser Guide Star system will be<br />

needed to achieve this sky coverage. NIFIRAOS is a MCAO system with conjugates at 0 and 12km.<br />

NFIRAOS is expected to deliver much improved image quality over a 2 arcmin field of view that will be used by<br />

an infrared multislit spectrometer. Expected AO performance over a 30 arcsec FoV and a 2 arcmin field are<br />

given in Table 3-1.. The LGS tomography is optimized for each FoV.<br />

Wide Field, Near-Diffraction-Limited, or multiple object adaptive optics (MOAO) will involve making AO<br />

correction of a number of small discrete angular regions (1-5 arcsec) distributed throughout a 5 arcmin field of<br />

view. This will allow diffraction-limited spectroscopy of 10-20 objects at a time.<br />

Moderate field, Diffraction-Limited, or Multi-conjugate Adaptive Optics (MCAO) which will have a well corrected<br />

30 arcsec field of view to allow precision photometry and imaging at the diffraction limit in the near IR. This role<br />

is initially filled by NFIRAOS.<br />

Small field diffraction-limited mid-IR (MIRAO) is the highest priority mid-IR science (5-28µm). It requires only a<br />

small field of view, as the science instrument will be an echelle spectrometer. High sky coverage is required.<br />

Planet Detection near the parent star will require Extreme Adaptive Optics. A proposed instrument, Planet<br />

Formation Imager will provide the additional AO capabilities and a coronagraph to make high contrast imaging<br />

Table 3-1: Enclosed Energy Fractions using NFIRAOS, inside of selected diameters of 50,<br />

100, 200 mas<br />

Field of view Wavelength band Image at center of field Image at edge of field<br />

50mas 100mas 200mas 50mas 100mas 200mas<br />

30 arcsec J (1.06-1.44µm) 0.60 0.62 0.66 0.58 0.59 0.62<br />

30 arcsec H (1.53-1.83µm) 0.73 0.74 0.78 0.70 0.72 0.76<br />

30 arcsec K (1.96-2.44µm) 0.79 0.80 0.84 0.78 0.79 0.82<br />

120 arcsec J (1.06-1.44µm) 0.30 0.38 0.52 0.15 0.26 0.46<br />

120 arcsec H (1.53-1.83µm) 0.48 0.54 0.63 0.30 0.38 0.57<br />

120 arcsec K (1.96-2.44µm) 0.61 0.66 0.72 0.46 0.51 0.64<br />

possible on relatively bright stars.<br />

<strong>TMT</strong> <strong>Construction</strong> <strong>Proposal</strong> 26

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