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TPF-I SWG Report - Exoplanet Exploration Program - NASA

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C HAPTER 1<br />

angled Three Telescope Nuller with a dedicated beam combiner spacecraft to alleviate the complexity of<br />

the beam relay, and sufficient asymmetry to improve the imaging properties.<br />

The focus at <strong>NASA</strong> was on improving the imaging properties of the array, which is important for<br />

separating the contributions from multiple planets, determining the orbit, and discriminating against<br />

lumps in the exozodiacal emission. This led to a rearrangement of the collectors in the Linear DCB to<br />

produce the X-Array – a configuration in which the nulling baselines lie along the short side of the<br />

rectangle and the imaging baselines (which determine the angular resolution) along the long dimension.<br />

The beams are relayed in a single hop from each collector to a central combiner. The decoupling of the<br />

nulling and imaging baselines makes the X-Array more flexible than other configurations. This flexibility<br />

was subsequently exploited to eliminate ‘instability noise’ with the ‘Stretched X-Array’ design. Instability<br />

noise—an analog of speckle noise in the coronagraph—arises from fluctuations in the path lengths,<br />

pointing, dispersion, etc. of the instrument, and drives the requirement on the null depth down to 10 -6 . The<br />

long imaging baselines of the Stretched X-Array give the planet signals a unique spectral signature that<br />

can be effectively separated from the instability noise, and they also greatly improve the angular<br />

resolution of the instrument.<br />

The configurations above are defined by the relative location of the collectors. Until recently, the<br />

combiner spacecraft was always located in the same plane as the collectors, normal to the direction to the<br />

target star. ESA then proposed the ‘Emma’ architecture, in which the combiner is moved out towards the<br />

star by about 1 km, and the collectors are reduced to a single spherical mirror. Most of the nulling<br />

configurations already described can be implemented in either the classic planar format or the out-ofplane<br />

Emma format. The Emma design offers significant advantages which are presently being studied<br />

independently by ESA and <strong>NASA</strong>. Preliminary results of these studies were first reported very recently,<br />

only in the later half of 2006, and are therefore not within the scope of this document. The appeal of the<br />

Emma design is primarily in its simplification of the telescope optics, eliminating the need for any<br />

deployables, and also in the design of the sunshields, which become folded into a hard shell—thereby<br />

reducing the risk of catastrophic failure. However, the simplification of the telescope optics increases the<br />

complexity of the beam combiner, and it currently is not known to what extent this will reduce the overall<br />

cost and risk of the mission. What is clear is that there exists obvious agreement in design principles<br />

between researchers at <strong>NASA</strong> and ESA, and the architectures for both <strong>TPF</strong>-I and Darwin appear to be<br />

converging in 2007.<br />

6

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