TPF-I SWG Report - Exoplanet Exploration Program - NASA
TPF-I SWG Report - Exoplanet Exploration Program - NASA
TPF-I SWG Report - Exoplanet Exploration Program - NASA
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C HAPTER 5<br />
5.4.4 Shear Metrology<br />
Shear metrology uses the same laser beam as the pointing system; the two systems are closely coupled.<br />
By placing a pupil stop at the FOR mirror, the alignment laser beam and the starlight have the same initial<br />
shear. Shear is first sensed after transfer to the next collector by a dichroic mirror with a set of lenses<br />
placed behind it (Figure 5-13). This dichroic lets through a portion of the 850-nm radiation, but the<br />
dichroic reflects most of it together with all the other useful light. The sensor output is run back to the<br />
transfer mirror on the first spacecraft to point the beam at the center of the dichroic shear sensor mirror.<br />
An identical method is used for transfer to the beamcombiner spacecraft. Once inside the beamcombiner,<br />
the shear is again sensed after the delay lines and corrected before entry to the adaptive nullers.<br />
5.4.5 Polarization Rotation<br />
Polarization-rotation metrology uses the same laser beam as the pointing system. The beam is initially<br />
polarized, and this forms a reference for beamtrain-induced rotations of the polarization angle. On arrival<br />
at the beamcombiner spacecraft, the beam is compressed and then passed through a K-mirror assembly,<br />
which allows the polarization angle to be rotated. A polarization-angle sensor is placed immediately after<br />
the K-mirror; thus, a loop can be formed to allow continuous correction of the polarization angle.<br />
Figure 5-14. Metrology scheme for simplified nulling beamcombiner.<br />
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