In this configuration, the K band light is split and sent to two
separate beam combiners. The fringes from the outputs of one combiner
are used to track the atmospheric piston at high rate (e.g. 200 Hz).
The fringes in the outputs of the other combiner are then
stable and longer integrations become possible (1 Hz frame rate
typically). Because both
combiners look at the same astrophysical object, the primary camera
(fast fringe tracker) sets the magnitude limit; the extra sensitivity
on the secondary combiner is used to enable spectral dispersion over
330 channels (R = 1700).
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