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Post-ionization, SNMS probability

The basic principle of e-beam SNMS as introduced by Lipinsky et al. in 1985 [3.60] is simple (Fig. 3.30) - as in SIMS, the sample is sputtered with a focused keV ion beam. SN post-ionization is accomplished by use of an e-beam accelerated between a filament and an anode. The applied electron energy Fe a 50 20 eV is higher than the range of first ionization potentials (IP) of the elements (4—24 eV, see Fig. 3.31). Typical probabilities of ionization are in the 0.01% range. SD and residual gas suppression is achieved with electrostatic lenses before SN post-ionization and energy filtering, respectively. [Pg.123]

Fig. 3.36. Experimental, Fe-related HF- calculated according to [3.74] from plasma SNMS sensitivity factors S(pe)x Ref [3.71] (salts) [3.72] alloys, [3.73] with elements X ordered according to round robins (r.r.). their post-ionization probabilities... Fig. 3.36. Experimental, Fe-related HF- calculated according to [3.74] from plasma SNMS sensitivity factors S(pe)x Ref [3.71] (salts) [3.72] alloys, [3.73] with elements X ordered according to round robins (r.r.). their post-ionization probabilities...
In SNMS, sputtered neutrals are post-ionized before they enter the mass spectrometer. In contrast to SIMS, SNMS does not suffer from the matrix effects associated with the ionization probability of sputtered particles. Here, the sensitivity for a cer-... [Pg.111]


See other pages where Post-ionization, SNMS probability is mentioned: [Pg.123]    [Pg.25]   
See also in sourсe #XX -- [ Pg.224 ]




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