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Relative beamsplitter efficiency

The relative beamsplitter efficiency of a film for unpolarized incident radiation is simply given by the average of the values for parallel and perpendicular polarized radiation ... [Pg.135]

The cracial parts of the system are the polychromator and the transfer optics. Polychromators and monochromators are usually optimised for high spectral resolution. This requires keeping the optical aberrations on the path through the polychromator smaller than the slit width. The result is a relatively low f-number, typically 1 3.5 to 1 8. The f-number limits the fraction of the fluorescence light that can be transferred into the entrance slit (see Sect. 7.2.4, page 279). Moreover, the efficiency of any grating is far less than 100%. Therefore some loss of photons on the way from the sample to the detector in unavoidable. A multiwavelength system based on a polychromator is less efficient than a system based on dichroic beamsplitters, but by far more efficient than a system that scans the spectrum by a monochromator. [Pg.86]


See other pages where Relative beamsplitter efficiency is mentioned: [Pg.23]    [Pg.23]    [Pg.302]    [Pg.355]    [Pg.100]    [Pg.164]    [Pg.400]    [Pg.138]    [Pg.248]   
See also in sourсe #XX -- [ Pg.135 ]




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