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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