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TMT Construction Proposal - Thirty Meter Telescope

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Fig 3-1: Atmospheric transmission for a high altitude site (Mauna Kea).<br />

3.2 <strong>Telescope</strong><br />

The telescope itself is the key to achieving our science goals. In this section we will describe the performance<br />

desired for the broad science objectives of this facility. The telescope is foremost an optical system, but it must<br />

also move to point to science targets, and it must provide suitable support of the science instruments that<br />

attach to it.<br />

3.2.1 Optical<br />

The telescope optics limit observations in a variety of ways and we describe the desired performance for the<br />

major categories.<br />

3.2.1.1 Optical Configuration<br />

The circumscribing circle around the primary is 30.0 m, and the useful<br />

collecting area is about 655 m 2 . The primary mirror (M1) is the entrance pupil<br />

of the telescope.<br />

We want a closely filled aperture to produce diffraction-limited images with the<br />

strongest central concentration of the light. When the starlight is faint<br />

compared to the background, the noise under the star image dictates the<br />

sensitivity. The time needed to reach a given S/N is proportional to<br />

b*(equivalent-noise area) where b is the background/unit area and the<br />

equivalent-noise area is the area that multiplies the background b to yield the<br />

variance in the estimate of a star intensity [2]. This is directly proportional to<br />

the needed observing time. The equivalent-noise area is<br />

α = 1/ ∫PSF 2 dA, where the PSF is normalized so ∫PSFdA = 1<br />

where PSF is the point spread function. For a given collecting area but with<br />

different configurations, α is the reciprocal of the observing efficiency. We indicate α for diffraction-limited<br />

observations with two configurations: a filled circular aperture and the segmented, <strong>TMT</strong> primary mirror (as<br />

shown in Fig. 3-2).<br />

aperture<br />

Filled aperture 1.31e-4 arcsec 2 (1.00)<br />

<strong>TMT</strong> 1.36e-4 arcsec 2 (1.04)<br />

equivalent-noise area for 1 μm (relative integration time)<br />

Fig 3-2: Pattern of 492<br />

segments of the primary<br />

mirror.<br />

The <strong>TMT</strong> primary mirror configuration is shown in Figure 3-2. The diffraction pattern profile of this mirror is<br />

shown in Figure 3-3.<br />

Experience with large telescopes has shown us that a single mirror (M1) giving images at prime focus is limiting<br />

for science instruments. A two-mirror telescope (M1+M2) giving a final focus at the Cassegrain focus (typically<br />

behind the primary) is more useful. An even more useful system employs an additional third fold flat (M3) that<br />

allows the Cassegrain focus to be folded over to the Nasmyth platforms. This design lets the telescope<br />

accommodate multiple science instruments with more room.<br />

<strong>TMT</strong> <strong>Construction</strong> <strong>Proposal</strong> 20

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