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TPF-C Technology Plan - Exoplanet Exploration Program - NASA

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Chapter 3<br />

are in progress with continuous improvements in the mask material, fabrication progress,<br />

algorithms, and testbed optics. Initial radiation tests show minimal HEBS mask performance<br />

degradation for the expected environmental exposure over mission lifetime.<br />

In addition to the HCIT implemented for evaluating mask performance and perfecting<br />

methodologies for star light suppression, an interferometer system has been developed at JPL to<br />

characterize HEBS mask material. This system, shown in Figure 3-2 incorporates 830, 785, 635,<br />

and 532 nm wavelength laser sources and a cooled CCD camera to capture interference fringe<br />

images. Algorithms have been developed to extract phase retardation/advance from such fringes<br />

from the various regions of different optical densities in the HEBS mask. This information is fed<br />

into models to validate experimental results. Reduction of error bars in measurement is an<br />

ongoing activity. Additionally, precision spectrophotometry and spectroscopic ellipsometry are<br />

employed to measure optical density and optical constants of the material as a function of<br />

wavelength.<br />

More recently Kuchner, Crepp, and Ge 2 have proposed replacement of the linear sinc 2 mask with<br />

an eighth order mask which is predicted to yield better tolerance to pointing instabilities and low<br />

order aberrations 3 .<br />

Focal plane binary masks: Focal plane masks of opaque and transparent regions<br />

lithographically formed on a metal film on glass are predicted to perform similar to the gray<br />

scale masks described above. Patterns of 1-sinc 2 , continuous sin 2 , and discontinuous sin 2 have<br />

Figure 3-2. Interferometric characterization of mask phase retardance.<br />

2 M.J. Kuchner, J. Crepp, and J. Ge, “Eighth-Order Image Masks for Terrestrial <strong>Plan</strong>et Finding,” Ap.J.<br />

628, pp. 466–73 (2005).<br />

30

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