Abstract:The Japan Proton Accelerator Research Complex (J-PARC) cesiated RF-driven H(-) ion source has been successfully operated for about 1 yr. By the world brightest level beam, the J-PARC design beam power of 1 MW was successfully demonstrated. Although no internal-RF-antenna failure, except for the once caused by an excess cesium due to a misoperation, occurred in the operation, many antennas failed in pre-conditionings for the first hundred days. The antenna failure rate was drastically decreased by using an ante… Show more
“…However, when scaled with the 12 min cesiation time, <0.6 mg/A·h of H -ions is a more likely amount. This is several orders of magnitude less than reported for similar [20,25] or other [31,32] sources. This means that the SNS ion source delivers at least 1200 H -ions per injected Cs atom, or more likely ~10 4 H -ions per injected Cs atom, and that usually without noticeable decay.…”
Section: A Record Run Illustratedmentioning
confidence: 49%
“…J-PARC's lower RF power and its high consumption of Cs explain their slightly different findings, including their preference of thicker coatings [25].…”
Section: The Successful Internal Antennasmentioning
“…However, when scaled with the 12 min cesiation time, <0.6 mg/A·h of H -ions is a more likely amount. This is several orders of magnitude less than reported for similar [20,25] or other [31,32] sources. This means that the SNS ion source delivers at least 1200 H -ions per injected Cs atom, or more likely ~10 4 H -ions per injected Cs atom, and that usually without noticeable decay.…”
Section: A Record Run Illustratedmentioning
confidence: 49%
“…J-PARC's lower RF power and its high consumption of Cs explain their slightly different findings, including their preference of thicker coatings [25].…”
Section: The Successful Internal Antennasmentioning
“…High-power and high-duty conditioning with cesium-abundant plasma for smaller emittances During the commissioning of a brand-new PCH, several RF-antennas are inevitably broken, probably due to the impurity elements sputtered from the PCH inner surface. The preconditioning procedure [13] has been applied to each RF-antenna. After failure of three RF-antennas, #7′ PCH with ventilation pathways for O-ring grooves successfully produces the 66 mA beam with the superior emittance shown in figure 13.…”
Section: Beam Apertures Of Pe and Ee For Higher Beam Intensity And Smmentioning
confidence: 99%
“…Similar emittances were measured two times for 66 mA beams produced using #2 PCH without ventilation pathways. All three degraded beams were produced after the preconditioning procedure [13], in which T PE was kept at the high value of 300°C for eight hours in the initial stage of the procedure, and a 24 h usual beam operation. The elimination of impurity elements with the high T PE is essential to reproduce the beams with similar emittances.…”
Section: Slight Water-fed Hydrogen For Lower Beam-divergence Angles Amentioning
confidence: 99%
“…The latter requirements have been satisfied using the superior internal RF-antenna developed at the Spallation Neutron Source (SNS) [3]. Several measures have been implemented to increase the beam brightness [4][5][6][7][8][9][10][11][12][13][14][15][16]. Almost all effective measures were found, in persistent experiments, to reproduce the accidentally produced H − ion beam with the record-breaking smallest emittances.…”
The H − ion beam intensity required for high-energy and high-intensity proton accelerators is continuously increasing. The required 95%-beam transverse normalized root mean square emittance (ε 95%rnmsx/y ) of the beam is around 0.25 πmm mrad for all accelerators. The Japan Proton Accelerator Complex (J-PARC) 400 MeV linear accelerator (LINAC) succeeded in accelerating the world's highest-class H − ion beam of 50 mA with a cesiated RF-driven H − ion source. This was achieved by increasing the beam brightness through the following measures
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