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Spectrometry surface charging

For a-spectrometry, silicon charged-particle detectors (surface-barrier detectors) have been used. They can be used over an extensive range of energies (20 kV-200 MeV). The inherent resolution of these surface-barrier detectors is surpassed only by that of magnetic spectrometers. [Pg.4133]

Surface-charging problems can also be minimised by the use of neutral beams to bombard surfaces instead of primary ions, a technique known as fast atom bombardment mass spectrometry (FABMS) [44-47]. A disadvantage of this type of process is that chemical information is limited to a spatial resolution of a few millimetres only, and no information is available on the spatial distribution of specific chemical moieties. [Pg.346]

In Dynamic Secondary Ion Ma s Spectrometry (SIMS), a focused ion beam is used to sputter material from a specific location on a solid surface in the form of neutral and ionized atoms and molecules. The ions are then accelerated into a mass spectrometer and separated according to their mass-to-charge ratios. Several kinds of mass spectrometers and instrument configurations are used, depending upon the type of materials analyzed and the desired results. [Pg.528]


See other pages where Spectrometry surface charging is mentioned: [Pg.17]    [Pg.148]    [Pg.148]    [Pg.145]    [Pg.508]    [Pg.78]    [Pg.2]    [Pg.166]    [Pg.42]    [Pg.21]    [Pg.148]    [Pg.205]    [Pg.202]    [Pg.2820]    [Pg.195]    [Pg.26]    [Pg.173]    [Pg.84]    [Pg.115]    [Pg.246]    [Pg.668]    [Pg.202]    [Pg.23]    [Pg.161]    [Pg.76]    [Pg.1812]    [Pg.554]    [Pg.265]    [Pg.32]    [Pg.32]    [Pg.230]    [Pg.236]    [Pg.409]    [Pg.384]    [Pg.71]    [Pg.13]    [Pg.27]    [Pg.242]    [Pg.366]    [Pg.25]    [Pg.304]    [Pg.21]    [Pg.60]    [Pg.364]    [Pg.19]    [Pg.175]    [Pg.381]   
See also in sourсe #XX -- [ Pg.346 ]




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