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Oral presentation

Operation status of the J-PARC negative ion source

Oguri, Hidetomo

no journal, , 

no abstracts in English

Oral presentation

Development of RF-driven negative hydrogen ion source for J-PARC

Ueno, Akira

no journal, , 

In order to achieve the design beam power of 1 MW, a negative hydrogen ion source with a peak beam current of 60 mA within horizontal and vertical 1.5 $${pi}$$mm$$cdot$$mrad emittances is under development. The beam extraction system is the same with the J-PARC ion source, which is using a lanthanum hexaboride (LaB$$_{6}$$) filament. The inner diameter of the plasma chamber is enlarged form 100 mm to 120 mm in order to install a water cooled plate attached to the plasma electrode (PE) and a cesium (Cs) injector. The end flange is modified to install the RF-antenna. A rod-filter flange is installed to produce a low-temperature plasma around the PE. For the conditions of the pulsed RF duty of 2.5% (1 ms $$times$$ 25 Hz), the air cooled PE (PE temperature of 120 $$^{circ}$$C) and opening the Cs valve for 4 min/day, a negative hydrogen ion beam with a peak beam current of more than 60 mA within 1.5 $${pi}$$mm$$cdot$$mrad emittances is successfully produced for more than 100 hours.

Oral presentation

Axial magnetic field effect for the J-PARC RF-driven ion source

Yamazaki, Saishun

no journal, , 

A cesium (Cs) seeded RF-driven H$$^{-}$$ ion source using an internal-antenna is under development for the Japan Proton Accelerator Research Complex (J-PARC). The J-PARC second stage requirements are an H$$^{-}$$ ion beam of 60 mA within normalized emittances of 1.5 $$pi$$mm$$cdot$$mrad both horizontally and vertically, and a flat top beam duty factor of 1.25% (500 $$mu$$s $$times$$ 25 Hz). An H$$^{-}$$ ion beam current of 77.5 mA with a flat top duty factor of 2% (800 $$mu$$s $$times$$ 25 Hz), whose approximately 90% (corresponding to approximately 70 mA) of each emittance is within 1.5 $$pi$$mm$$cdot$$mrad, is successfully extracted from it. The experimental results of axial magnetic field (AMF) optimization with an axial magnetic field correction (AMFC) coil, which significantly enhances the H$$^{-}$$ ion beam current by 10% typically, are presented in this meeting.

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