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potential between the negatively biased cathode and the anode. Free electrons in
      the gas are accelerated toward the positively biased anode by the resulting poten-
      tial gradient. These free electrons collide with gaseous species, producing gas-
      phase ions. Positive ions are accelerated toward and impinge on the negatively
      biased electrode. On impact, a variety of secondary species are liberated, includ-
      ing electrons and species formed from the cathode material. The ions and atoms
       from the cathode have analytical utility since they represent the sample. The entire
      process is considered self-sustaining on the basis that electrons are created at
       the cathode to replace those lost at the anode. Hence, no external ionization is
       required [25].
           The relationship between current and operating voltage is a characteristic by
       which gas discharges can be identified. Figure 2.1 illustrates this relationship;
       several types of  discharges are identified along with  their associated electrical
       behavior [26]. In the   to 10-15-A region (regions B and C) are the electrical
       discharges requiring an external source of  ionizing radiation to maintain current
       flow [24]. A feature of these discharges is the lack of luminosity resulting from the
       small number  of  collisional excitation processes. At  10-lo A  the  discharges
       possess the ability to sustain current flow independently of  external assistance,







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                Voltage versus current characteristics of gas discharges. (From Ref. 26.)
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