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Wavelength modulation background correction

All of the flicker noises can be effectively eliminated by the use of double-beam optics in conjunction with a background correction system such as Zeeman splitting or a well-aligned (or wavelength-modulated) continuum source. Thus the ultimate limiting noise in atomic absorption is source shot noise, which can be reduced (relative to total source intensity or I, ) by increasing the source intensity, up to the point of optical saturation. [Pg.119]

The possibility of modulating the emitted wavelength of DLs at GHz frequencies by the modulation of the diode current allows one to reduce the low-frequency (flicker) noise in the baseline, which again improves the detection limit. Emission wavelength modulation also permits to correct for unspecific background absorption, thereby improving the selectivity of the technique. [Pg.440]

Background correction by wavelength-modulation is not widely used, but seems to have considerable potential for simultaneous multi-element AAS with continuum sources. Alternatively, high-resolution echelle gratings may be used that can detect both the elemental line and the background at the same time. [Pg.462]


See other pages where Wavelength modulation background correction is mentioned: [Pg.18]    [Pg.37]    [Pg.281]    [Pg.156]    [Pg.157]    [Pg.462]    [Pg.237]    [Pg.237]    [Pg.237]    [Pg.2459]    [Pg.45]    [Pg.156]    [Pg.157]    [Pg.427]    [Pg.427]    [Pg.169]    [Pg.170]    [Pg.11]    [Pg.59]    [Pg.318]    [Pg.519]    [Pg.378]    [Pg.571]   
See also in sourсe #XX -- [ Pg.462 ]




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