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TPF-I SWG Report - Exoplanet Exploration Program - NASA

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D ESIGN AND A R C H I T E C T U R E T RADE S TUDIES<br />

4.6 Beam Combiner Design<br />

In nulling interferometry, excess starlight is blocked using an interferometric cancellation technique,<br />

improving the star-to-planet contrast ratio to enable planet detection over an observation time typically of<br />

several hours. To reduce the stellar leakage signal to a level comparable to the zodiacal background the<br />

nuller should be capable of reaching null depths of at least 10 -5 . To reach deep nulls, a number of<br />

parameters must be controlled, some inside the nuller and some in other associated systems. An important<br />

feature of a successful nulling beam combiner will be identical treatment of both input beams in terms of<br />

phase shifts, reflections and transmissions, angles of incidence, polarizations, etc. Different nuller designs<br />

are being tested in the laboratory and in the field. A modified Mach-Zehnder design (MMZ) has been<br />

deployed on the Keck telescopes, and this design seeks to achieve a high degree of symmetry in the beam<br />

combination by causing each input beam to be both transmitted once and reflected once from nearidentical<br />

beamsplitters (this design achieved 2 million to 1 laser nulls at 10.6 μm).<br />

A different design (also using conventional beamsplitters), the rooftop nuller, was built at JPL for SIM<br />

and achieved high performance nulls (laser transient nulls at 633 nm near 10 -6 and 18% bandwidth redlight<br />

nulls of 10 -4 ) in the visible waveband. A newer concept, the fiber beam combiner is currently being<br />

tested in the laboratory for deployment on a large ground-based telescope. This design seeks to achieve<br />

high beam symmetry by dispensing with the beamsplitters and combining the incoming beams directly on<br />

the tip of a single-mode optical fiber, and this design has already achieved laser nulls of 10 5 in the visible.<br />

Bright<br />

outputs<br />

Beamsplitter 4<br />

Common<br />

mirrors<br />

Nulled<br />

outputs<br />

Inner mirror<br />

Input beams<br />

Beamsplitter 1<br />

Outer mirror<br />

Figure 4-11. Modified Mach-Zehnder nuller used on Keck Telescopes.<br />

73

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