2000
DOI: 10.1103/physreve.61.3015
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Highly charged ion densities and ion confinement properties in an electron-cyclotron-resonance ion source

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Cited by 90 publications
(115 citation statements)
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“…The high-energy component has a typical temperature of several tens of keVs [3] while the low-energy component has a much lower value, around 1 keV. Measured temperatures for the high energy electron population range from 5 to 13 keV for an ECRIS operated at 2.45 GHz [6,7], 40-60 keV for a CAPRICE source operated at 10 GHZ [13], and up to 100 keV for an ECRIS operated at 18 and 28 GHz [3,10]. As in the measurements cited above, our study is sensitive to the high-energy electron component due to our detection energy range of ∼ 20 − 120 keV.…”
Section: Evaluation Of the Plasma Characteristics A Bremsstrahlmentioning
confidence: 99%
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“…The high-energy component has a typical temperature of several tens of keVs [3] while the low-energy component has a much lower value, around 1 keV. Measured temperatures for the high energy electron population range from 5 to 13 keV for an ECRIS operated at 2.45 GHz [6,7], 40-60 keV for a CAPRICE source operated at 10 GHZ [13], and up to 100 keV for an ECRIS operated at 18 and 28 GHz [3,10]. As in the measurements cited above, our study is sensitive to the high-energy electron component due to our detection energy range of ∼ 20 − 120 keV.…”
Section: Evaluation Of the Plasma Characteristics A Bremsstrahlmentioning
confidence: 99%
“…[13]). This distribution can be represented as the sum of two Maxwellian distributions f Mw (E) corresponding to a low-energy and high-energy electron populations, where…”
Section: Evaluation Of the Plasma Characteristics A Bremsstrahlmentioning
confidence: 99%
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