2019
DOI: 10.1063/1.5128458
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Wide-aperture dense plasma fluxes production based on ECR discharge in a single solenoid magnetic field

Abstract: Results of experimental investigation of the ECR discharge in a single coil magnetic field as an alternative to RF and helicon discharges for wide-aperture dense plasma fluxes production are presented. A possibility of obtaining wide-aperture high density hydrogen plasma fluxes with homogenous transverse distribution was demonstrated in such a system. The prospects of using this system for obtaining high current ion beams are discussed.

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Cited by 7 publications
(2 citation statements)
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“…The electric field on the order of 1 MV/cm would have been needed to form the ion beam, which is not technically feasible. Despite the plasma being highly collisional, its flux follows the magnetic field in the region of interest [31], allowing for easy way to tune the flux density in the extraction region by changing its position relative to the magnetic field. Thus, the plasma electrode was placed 100 mm downstream the beam line, where the trap magnetic field and, therefore, the plasma flux density decreased by a factor of 7 down to 1 A/cm 2 , which falls within the voltage range available at the facility (up to 100 kV).…”
Section: Methodsmentioning
confidence: 99%
“…The electric field on the order of 1 MV/cm would have been needed to form the ion beam, which is not technically feasible. Despite the plasma being highly collisional, its flux follows the magnetic field in the region of interest [31], allowing for easy way to tune the flux density in the extraction region by changing its position relative to the magnetic field. Thus, the plasma electrode was placed 100 mm downstream the beam line, where the trap magnetic field and, therefore, the plasma flux density decreased by a factor of 7 down to 1 A/cm 2 , which falls within the voltage range available at the facility (up to 100 kV).…”
Section: Methodsmentioning
confidence: 99%
“…Neutrons were generated through D−D-reaction with the yield of fast neutrons (2.5 MeV) 1.2 • 10 10 s −1 at the beam current 50 mA and energy 75 keV in pulsed mode with pulse width of about 1 ms [26]. This neutron generator is considered not only for BNCT applications [22,27], but also for neutron tomography [28][29][30]26].…”
Section: Introductionmentioning
confidence: 99%