TPF-C Technology Plan - Exoplanet Exploration Program - NASA
TPF-C Technology Plan - Exoplanet Exploration Program - NASA
TPF-C Technology Plan - Exoplanet Exploration Program - NASA
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Structural, Thermal, and Spacecraft <strong>Technology</strong><br />
Laser truss<br />
Interferometer<br />
Metering truss<br />
Figure 4-18. Sunshield/isothermal cavity performance testbed evolved to test the optical<br />
stability of a quarter-scale mirror representative of the <strong>TPF</strong>-C primary mirror.<br />
Surface changes of 0.2–0.4 nm can be tolerated during an exposure, up to 24 hours and including<br />
a dither maneuver. The test will therefore be looking for thermally induced surface deformations<br />
of this size at low spatial frequencies. Relevant heritage for measurement accuracies of this level<br />
is only currently being established. Researchers at the National Institute of Standards and<br />
<strong>Technology</strong> have measured the surface of a 30-cm flat mirror at room temperature with an error<br />
of 0.2 nm (not yet published). Blake et al. 33 measured a 17-cm flat mirror at 30 K with an error<br />
of 1 nm. The test optics in these cases were comparatively small, allowing variables in the test to<br />
be tightly controlled. Measurements on a larger mirror (~1.4 m), the Advanced Mirror System<br />
Demonstrator (AMSD), at cryogenic temperatures, have error bars of 14 nm. 34 The test proposed<br />
here on a 2-m sphere represents a challenge to current measurement capabilities. We propose to<br />
largely eliminate noise in our measurements due to the support structure between the test mirror<br />
and the wavefront sensing device by employing a laser truss to control a hexapod support of the<br />
wavefront sensor. This technology is proposed to control the position of the secondary mirror in<br />
the <strong>TPF</strong>-C telescope. A subscale demonstration is discussed in Section 4.2.1. An independent<br />
laser system will measure the effectiveness of the truss. In addition tight thermal control of the<br />
wavefront sensor assembly and frequency control of the light source will reduce noise from these<br />
sources. Detector noise will be minimized. This test does not require a very accurate figure; λ/20<br />
will suffice since the objective of the test is to track changes in the surface shape. However, good<br />
33 Blake, P. et al., “NIRSpec Mirrors Cryogenic Testing Final Report,” Goddard Space Flight Center,<br />
2005.<br />
34 Reardon, P.J et al., “Advanced Mirror System Demonstrator Cryogenic Error Test Budget,” SPIE<br />
Proceedings 4850, 2003.<br />
79