2015
DOI: 10.1063/1.4916417
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Numerical and experimental study of atomic transport and Balmer line intensity in Linac4 negative ion source

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Cited by 11 publications
(16 citation statements)
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“…8 provided a description of the RF-plasma heating process, Shibata et.al 9 calculated the plasma light emission and, across a wide range of plasma conditions, Mochalskyy et. al.…”
Section: Discussionmentioning
confidence: 99%
“…8 provided a description of the RF-plasma heating process, Shibata et.al 9 calculated the plasma light emission and, across a wide range of plasma conditions, Mochalskyy et. al.…”
Section: Discussionmentioning
confidence: 99%
“…Giant RF-ICP sources for N-NBI plasma heating in fusion applications have been developed [4] and further scale-up is now undertaken for the International Thermonuclear Experimental Reactor N-NBI system [3]. Recent progress in the modeling of such a RF-ICP giant H − source for fusion plasma applications has been reported in [32 and reference therein].In this paper, we focus on a series of the modeling studies in [33][34][35] of the compact RF-ICP H − source for the CERN Linac4 accelerator [8]. In RF-ICP, operation mode is generally classified into two modes [10,13]: in the relatively low density regime, the high voltage across the coil couples to the plasma capacitively (E-mode), while in the relatively high-density regime, the discharge is sustained by the electric field induced by the radio frequency (RF) current in the coil (H-mode).…”
mentioning
confidence: 99%
“…In RF-ICP, operation mode is generally classified into two modes [10,13]: in the relatively low density regime, the high voltage across the coil couples to the plasma capacitively (E-mode), while in the relatively high-density regime, the discharge is sustained by the electric field induced by the radio frequency (RF) current in the coil (H-mode). A sharp transition from the E-mode to the H-mode (E-H transition) has been frequently observed in various experiments [13,34,35]. Understanding of the E-H transition is one of the key issues especially for the impedance matching between the RF-system and plasma loading, because the plasma characteristics and the resultant plasma loading impedance significantly change before and after the transition.…”
mentioning
confidence: 99%
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“…The asymmetric emission is associated with the capacitive coupling driving the plasma. As shown in [26] the line integrated light emission, reconstructed from a collision-radiative model, indicates that the higher peak results from the E-field pushing the electrons towards the view port (figure 6) while the smaller peak to the plasma centred in the plasma chamber ( figure 7). The main contribution to the light intensity is the distance of the photon emission to the view port and the emission roughly scales with the local electron density.…”
Section: Resultsmentioning
confidence: 91%