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where Dx is the minimum feature size used in the focal plane. Comparing with Eqns. (9.42), (9.23), and (9.11), we nd that the FP spectrometer ef ciency substantially exceeds the slit and FT ef ciency. Assuming that the order of the coded aperture is N % V 1/3/Dx, the ef ciency of the FP and coded aperture instruments is approximately comparable. As with previous systems, the ef ciency does not tell the whole story for the FP spectrometer. Operating over a single free spectral range, the etalon is effectively a narrow-pass spectral lter. Only one spectral channel is detected for each value of u. Thus, the spectrally averaged throughput is reduced by a factor of 1/F relative to dispersive and multiplexed interferometric systems. An FP system thus needs F times greater ef ciency to achieve the same SNR as a dispersive system. This comparison is also not quite fair, however, because the spectral resolution that one can obtain from an FP system is extraordinary, and the spectral range is typically quite limited. The high spectral resolution is typical of resonant systems generally and of systems resonant with modes oscillating along the longitudinal axis speci cally. Overcoming the limited spectral range of the FP spectrometer requires only that we expand our mathematical horizons. Multiplex Fabry Perot spectroscopy solves Eqn. (9.57) for S0 (n) spanning multiple free spectral ranges. We consider multiplex instruments here from a somewhat different perspective than in previous studies [52,117,231]. Equation (9.57) is a Fredholm integral equation of the rst kind with a symmetric kernel. Such equations may be inverted by standard methods [134]. In spectroscopy, where one typically need estimate only a few thousand channels, direct algebraic methods are convenient.



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