Pulse duration of the ITER-relevant high power density hydrogen negative ion beams at 1 MeV has been successfully extended from 0.4 s to 60 s by using a prototype Multi-Aperture and Multi-Grid accelerator for the ITER and JT-60SA neutral beam systems. This significant progress was achieved based on developments of technology for the design of a voltage holding capability and improvement of a beam optics, which are directly applicable to ITER and JT-60SA. In the design of the voltage holding capability, one of critical remaining issues was a multi-grid effect. This was experimentally investigated by using a multi-grid configuration. This result was also applied to improve the beam optics by tuning the acceleration gap. In addition, the extra...
The beam source of neutral beam heating/current drive system for ITER is needed to accelerate the ne...
One of the objectives of the BNL Neutral Beam Development Group is to accelerate negative hydrogen i...
The first emittance measurement of the high power density negative ion beam at target perveance cond...
Pulse duration of the ITER-relevant high power density hydrogen negative ion beams at 1 MeV has been...
A long pulse acceleration of high-power-density hydrogen negative ion beams of 184 MW/m2 (0.97 MeV, ...
Long pulse acceleration of hydrogen negative ion beams with the power density over 70 MW/m2 and the ...
High power density of hydrogen negative ion beams with over 70 MW/m2 at the energy of 500 keV has be...
In the negative-ion-based neutral beam injector (N-NBI) of JT-60SA, a hydrogen negative ion beam wit...
ITER neutral beam injector (NBI) is required to produce 1 MeV 16.5 MW neutral beams for 3600 seconds...
High energy and high power negative ion sources and accelerators have been developed for neutral bea...
Abstract. The paper reports the progress of R&D toward the ITER neutral beam (NB) system at Japa...
The negative ion neutral beam system now operating on JT-60U was the first application of negative i...
Abstract. The paper reports the progress of R&D toward the JT-60SA at Japan Atomic Energy Agency...
Abstract: In the ITER NB, conventional gas insulated beam source (GIBS) cannot be utilized because o...
Abstract. IPP Garching has successfully developed a RF driven negative ion source for the ITER neutr...
The beam source of neutral beam heating/current drive system for ITER is needed to accelerate the ne...
One of the objectives of the BNL Neutral Beam Development Group is to accelerate negative hydrogen i...
The first emittance measurement of the high power density negative ion beam at target perveance cond...
Pulse duration of the ITER-relevant high power density hydrogen negative ion beams at 1 MeV has been...
A long pulse acceleration of high-power-density hydrogen negative ion beams of 184 MW/m2 (0.97 MeV, ...
Long pulse acceleration of hydrogen negative ion beams with the power density over 70 MW/m2 and the ...
High power density of hydrogen negative ion beams with over 70 MW/m2 at the energy of 500 keV has be...
In the negative-ion-based neutral beam injector (N-NBI) of JT-60SA, a hydrogen negative ion beam wit...
ITER neutral beam injector (NBI) is required to produce 1 MeV 16.5 MW neutral beams for 3600 seconds...
High energy and high power negative ion sources and accelerators have been developed for neutral bea...
Abstract. The paper reports the progress of R&D toward the ITER neutral beam (NB) system at Japa...
The negative ion neutral beam system now operating on JT-60U was the first application of negative i...
Abstract. The paper reports the progress of R&D toward the JT-60SA at Japan Atomic Energy Agency...
Abstract: In the ITER NB, conventional gas insulated beam source (GIBS) cannot be utilized because o...
Abstract. IPP Garching has successfully developed a RF driven negative ion source for the ITER neutr...
The beam source of neutral beam heating/current drive system for ITER is needed to accelerate the ne...
One of the objectives of the BNL Neutral Beam Development Group is to accelerate negative hydrogen i...
The first emittance measurement of the high power density negative ion beam at target perveance cond...