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Previous ionization systems have generally failed to achieve a controlled uniform rate of ionization. These systems suffer from energy dependence, catastrophic electrical discharge, and non-uniform distribution of energy along the length of the charging electrode.
The previously known techniques used to measure the charging efficiency of a region (i.e., the current flowing per unit area), require that energy be continuously applied to the area being charged in order to maintain a constant current flow. Currents obtained from a constant applied potential may vary across the surface of the chamber if the local current density varies over the area. A localized electrode will accumulate charge according to its ability to accept charges in the DC field and its ability to transport charges to an electrical ground. This accumulation of charge is caused by an increase in local potential over a short distance. This accumulation of charge causes the local field and thus the current density to increase locally. This increase in current density will limit the current in those regions of the chamber. This limitation in current density will appear as an apparent variation in current in a constant applied potential configuration.
Known spectrometers do not control the ionization and charging parameters nor do they calculate or predict ion current as a function of ionization parameters or temporal parameters. Also, no method has been disclosed to use ion kinetic theory in order to predict ion current as a function of ionization parameters or temporal parameters.
It is therefore an object of the present invention to provide a means to control the energy (i.e., electron, positron, or photon) used for a plurality of ionizations.
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