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Fig. 1

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Geometry of a simple slitless spectrograph in the plane orthogonal to the CCD (top) and parallel to the CCD (bottom). A convergent beam with incident angle θ0 is focused on a CCD at position r0 = (x0,y0), but also passed through a grating with Neff grooves per millimetre at a distance DCCD above the CCD. The beam is deflected at an angle θ(λ) along the mean dispersion axis u, which forms an angle α with respect to the CCD x axis, but is focused somewhere above the sensor. Atmospheric refraction adds a supplementary dispersion along and transversally to the mean dispersion axis.

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