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Diffraction-limited grating monochromator

This function is shown in Figure 2.7. As we saw from the discussion of the Rayleigh criterion of resolution, this is also the shape of the ILS function of a diffraction-limited grating monochromator. It can be seen that the amplitude of the sidelobes has been considerably reduced from that of the sidelobes for the sine function. Suppression of the magnitude of these oscillations is known as apodization, and functions such as Ai(S), which weight the interferogram for this purpose, are known as apodization functions. [Pg.32]

See other pages where Diffraction-limited grating monochromator is mentioned: [Pg.7]    [Pg.123]    [Pg.96]    [Pg.63]    [Pg.143]    [Pg.6526]    [Pg.140]    [Pg.91]    [Pg.92]    [Pg.99]    [Pg.347]    [Pg.52]    [Pg.6525]    [Pg.92]    [Pg.38]    [Pg.36]    [Pg.77]    [Pg.384]    [Pg.106]    [Pg.106]    [Pg.384]    [Pg.323]    [Pg.38]    [Pg.289]    [Pg.300]    [Pg.81]    [Pg.635]    [Pg.194]    [Pg.494]    [Pg.51]    [Pg.816]    [Pg.32]    [Pg.277]    [Pg.351]    [Pg.804]    [Pg.64]   
See also in sourсe #XX -- [ Pg.31 , Pg.32 ]



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Monochromate

Monochromator

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