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Multichannel spectrometers above

The graphical method described above using the x-ray tube current can also be employed with the multichannel analyzer systems in energy-dispersive spectrometers. The filter technique cannot be used, however, since it distorts the measured spectrum. The general equation (4.124) must be used. Fortunately, the value of the ratio R/p(E) can be measured directly from the observed spectrum on the multichannel analyzer at low counting rates. This allows the true deadtime to be calculated from Eq. (4.125). [Pg.189]


See other pages where Multichannel spectrometers above is mentioned: [Pg.278]    [Pg.241]    [Pg.30]    [Pg.435]    [Pg.21]    [Pg.51]    [Pg.290]    [Pg.127]    [Pg.653]    [Pg.79]    [Pg.127]    [Pg.52]    [Pg.236]    [Pg.33]    [Pg.624]    [Pg.198]    [Pg.1812]    [Pg.1631]    [Pg.39]    [Pg.34]    [Pg.477]    [Pg.269]   
See also in sourсe #XX -- [ Pg.245 ]




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Multichannel

Multichannel spectrometers

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