2020
DOI: 10.1063/1.5131302
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Achievement of high power and long pulse negative ion beam acceleration for JT-60SA NBI

Abstract: Long pulse acceleration of hydrogen negative ion beams with the power density over 70 MW/m2 and the pulse length over 100 s has been demonstrated for the first time by using a multi-aperture 3-stage accelerator. Such long pulse acceleration was achieved by integrating the design of beam optics and voltage holding capability to meet the requirements of JT-60SA. By using the newly designed accelerator for JT-60SA, voltage holding at 500 kV with beam acceleration was stably sustained even after 5 g of cesium was … Show more

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Cited by 17 publications
(14 citation statements)
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“…It was found that the PG temperature strongly affects the measured cesium density, which, during plasma pulses, increases by a factor of 3 when decreasing T PG from 140 • C to 80 • C. If the cesium density before the grid surface is associated with the cesium coverage on the surface, this suggests that, within this range, the lower temperature would be more suitable for negative ion production, as it was also shown by the negative ion current. This result appears different from the findings in filament-based sources, which instead operate at significantly higher temperatures [23]. However, it should be mentioned that the temperature of the PG mask, which is not temperature-controlled, is unknown, yet certainly higher than the PG one; so the effective PG temperature might be higher than indicated.…”
Section: First Cesium Campaign In Spidercontrasting
confidence: 74%
“…It was found that the PG temperature strongly affects the measured cesium density, which, during plasma pulses, increases by a factor of 3 when decreasing T PG from 140 • C to 80 • C. If the cesium density before the grid surface is associated with the cesium coverage on the surface, this suggests that, within this range, the lower temperature would be more suitable for negative ion production, as it was also shown by the negative ion current. This result appears different from the findings in filament-based sources, which instead operate at significantly higher temperatures [23]. However, it should be mentioned that the temperature of the PG mask, which is not temperature-controlled, is unknown, yet certainly higher than the PG one; so the effective PG temperature might be higher than indicated.…”
Section: First Cesium Campaign In Spidercontrasting
confidence: 74%
“…Although the ITER targets were not demonstrated up to now, the achieved combination of CW extraction pulse length and current density represents a huge step forward compared to previous results and to the results of other test facilities (see for example [18]).…”
Section: Upgrade Of Elise To Cw Extraction and First Resultsmentioning
confidence: 91%
“…Then, the gap length was changed from 75/65/55 mm in the original to all 85 mm. (B) Suppression of generation of the diverged beam and secondary electrons inside the EXG [8,9,15]: these are the cause of the grid heat load. In the beam analysis carried out to understand these issues, the negative ions extracted from the PG with a diameter of 14 mm are converged between the PG and the EXG due to the extraction voltage, and then they spread inside the 17 mm thick EXG.…”
Section: Accelerator and Modification Pointsmentioning
confidence: 99%
“…In section 4, the filament break and its protection are reported. Section 5 shows a demonstration of the beam acceleration toward 500 keV, 130 A m −2 for 100 s [15]. Through this beam acceleration test, influences of the Cs leaked to the accelerator are also investigated and discussed.…”
Section: Introductionmentioning
confidence: 99%