2013
DOI: 10.1063/1.4792772
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Analysis of the double-ion plasma in the extraction region in hydrogen negative ion sources

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Cited by 8 publications
(14 citation statements)
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“…In various Cs-seeded negative ion sources, an 'ion-ion plasma' layer which mainly consists of positive and negative ions has been observed in front of the PG [51,52,98,99]. Especially, recent experiments on the ion-ion plasma in [51] triggered a series of 2D ES-PIC modeling studies [39][40][41][42] in order to find the answer for the questions: (i) 'why such a thick ion-ion plasma layer is produced under the H − SP? ', and 'from where H − ions are extracted?…”
Section: Extraction Physicsmentioning
confidence: 99%
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“…In various Cs-seeded negative ion sources, an 'ion-ion plasma' layer which mainly consists of positive and negative ions has been observed in front of the PG [51,52,98,99]. Especially, recent experiments on the ion-ion plasma in [51] triggered a series of 2D ES-PIC modeling studies [39][40][41][42] in order to find the answer for the questions: (i) 'why such a thick ion-ion plasma layer is produced under the H − SP? ', and 'from where H − ions are extracted?…”
Section: Extraction Physicsmentioning
confidence: 99%
“…A series of 2D3V ES-PIC (two-dimensional in real space and three-dimensional velocity space, ES-PIC) modeling has been done in [36][37][38][39][40][41][42]. A reduced-size-scaling has been adopted to save the computational cost by keeping important normalized parameters the same as those in the real system [36,[38][39][40][41][42], e.g., normalized Larmor radius r L, j Lj * r = / collisionality parameter L, jk jk * l l = / where L is the characteristic scale length of the real system, while r Lj and jk l are the Larmor radius and collision mean free path, respectively. The symbols j and k denote particle species.…”
Section: Introductionmentioning
confidence: 99%
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