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TPF-I SWG Report - Exoplanet Exploration Program - NASA

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C HAPTER 6<br />

Figure 6-1. The State of the Art of Nulling Interferometry: Laboratory results showing null depth as a<br />

function of bandwidth for experiments at visible, infrared, and mid-infrared wavelengths. Results that are<br />

plotted with a zero bandwidth are laser measurements. Almost all results are limited to a singlepolarization<br />

input. All but one of the results are from two-beam nulling interferometers. The result by<br />

Martin et al. (2005) is from the four-beam Planet Detection Testbed, described later in this Section. The<br />

result by Gappinger (2006) is an unpublished result from the Achromatic Nulling Testbed. The result by<br />

Peters (2007) is a preliminary and unpublished result from the Adaptive Nuller. The literature references,<br />

where available, are listed at the end of this chapter.<br />

<strong>TPF</strong>-I are the experiments that have been conducted at mid-infrared wavelengths, which are indicated by<br />

the red circles in the plot.<br />

From the results to date, we can draw the following conclusions.<br />

1. Experiments have shown that achromatic effects (predominantly pathlength variations) can be<br />

controlled in the lab at a level that allows rejection ratios better than 1,000,000:1 to be achieved<br />

repeatedly. This level of performance exceeds the requirements for <strong>TPF</strong>-I. Narrow-bandwidth<br />

laser nulls have been attained with mid-infrared rejection ratios of 2,000,000:1 and at visible<br />

wavelengths of 10,000,000:1.<br />

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