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TPF-I SWG Report - Exoplanet Exploration Program - NASA

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<strong>TPF</strong>-I F L I G H T B ASELINE D ESIGN<br />

once. Additionally, the completeness per star varies in the new simulation. In general, the closer stars are<br />

more complete than those that are further away. The completeness per star as a function of angular radius<br />

to the mid-HZ and distance to the star is shown in Fig. 5-29.<br />

The completeness calculations for this simulation are lower than previous estimations because there is<br />

now more fidelity in the current model. We compute planet flux as a function of HZ distance in the new<br />

simulations. Because there is a sharp fall-off in the mid-IR flux in the outer HZ, fewer outer HZ planets<br />

are observable. Furthermore, if we map completeness across the HZ, there is a marked fall-off of<br />

completeness as a function of pseudo-planet distance. Future work includes a study of the effect of forced<br />

revisits on completeness.<br />

5.9 References<br />

Lay, O. P., “Imaging properties of rotating nulling interferometers,” Appl. Opt. 44, 5859–5871 (2005).<br />

Martin, S., “The flight instrument design for the Terrestrial Planet Finder Interferometer,” Techniques and<br />

Instrumentation for Detection of <strong>Exoplanet</strong>s II, Proc. SPIE 5905, edited by D. R. Coulter, 21–35<br />

(2005).<br />

129

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