Abstract:We report on the characteristics of the electronegative plasma in a large-scale hydrogen negative ion (H(-)) source. The measurement has been made with a time-resolved Langmuir probe installed in the beam extraction region. The H(-) density is monitored with a cavity ring-down system to identify the electrons in the negative charges. The electron-saturation current decreases rapidly after starting to seed Cs, and ion-ion plasma is observed in the extraction region. The H(-) density steps down during the beam e… Show more
“…The result shows that n H − in the upstream region away from the plasma meniscus has been reduced by applying the extraction voltage. This result shows the similar tendency to the result of the experiments [6,7]. At the same time, electorstatic oscillation has been observed in the extraction region.…”
Section: Resultssupporting
confidence: 79%
“…However, the extraction mechanisms have not been completely clarified yet. Double-ion plasma layer, which is consisting of H + and H − ions, has been observed in the vicinity of Plasma Grid (PG) of Cs-seeded H − negative ion sources, experimentaly [6]. Recent experiments show that H − density n H − in the upstream region away from the plasma meniscus (H − emitting surface) has been reduced by applying the extraction voltage [6,7].…”
Section: Introductionmentioning
confidence: 99%
“…Double-ion plasma layer, which is consisting of H + and H − ions, has been observed in the vicinity of Plasma Grid (PG) of Cs-seeded H − negative ion sources, experimentaly [6]. Recent experiments show that H − density n H − in the upstream region away from the plasma meniscus (H − emitting surface) has been reduced by applying the extraction voltage [6,7]. This fact indicates that the transport of H − ions in the double-ion plasma layer even far from the PG are affected by the extraction voltage, although the extraction voltage is shielded by the Debye shield effect.…”
Study of ion-ion plasma formation in negative ion sources by a three-dimensional in real space and three-dimensional in velocity space particle in cell model Journal of Applied Physics 119, 023302 (2016) Abstract. We have developed a 2D3V-PIC model of the extraction region, aiming to clarify the basic extraction mechanism of H − ions from the double-ion plasma in H − negative ion sources. The result shows the same tendency of the H − ion density n H − as that observed in the experiments, i.e., n H − in the upstream region away from the plasma meniscus (H − emitting surface) has been reduced by applying the extraction voltage. At the same time, relatively slow temporal oscillation of the electric potential compared with the electron plasma frequency has been observed in the extraction region. Results of the systematic study using a 1D3V-PIC model with the uniform magnetic field confirm the result that the electrostatic oscillation is identified to be lower hybrid wave. The effect of this oscillation on the H − transport will be studied in the future.
“…The result shows that n H − in the upstream region away from the plasma meniscus has been reduced by applying the extraction voltage. This result shows the similar tendency to the result of the experiments [6,7]. At the same time, electorstatic oscillation has been observed in the extraction region.…”
Section: Resultssupporting
confidence: 79%
“…However, the extraction mechanisms have not been completely clarified yet. Double-ion plasma layer, which is consisting of H + and H − ions, has been observed in the vicinity of Plasma Grid (PG) of Cs-seeded H − negative ion sources, experimentaly [6]. Recent experiments show that H − density n H − in the upstream region away from the plasma meniscus (H − emitting surface) has been reduced by applying the extraction voltage [6,7].…”
Section: Introductionmentioning
confidence: 99%
“…Double-ion plasma layer, which is consisting of H + and H − ions, has been observed in the vicinity of Plasma Grid (PG) of Cs-seeded H − negative ion sources, experimentaly [6]. Recent experiments show that H − density n H − in the upstream region away from the plasma meniscus (H − emitting surface) has been reduced by applying the extraction voltage [6,7]. This fact indicates that the transport of H − ions in the double-ion plasma layer even far from the PG are affected by the extraction voltage, although the extraction voltage is shielded by the Debye shield effect.…”
Study of ion-ion plasma formation in negative ion sources by a three-dimensional in real space and three-dimensional in velocity space particle in cell model Journal of Applied Physics 119, 023302 (2016) Abstract. We have developed a 2D3V-PIC model of the extraction region, aiming to clarify the basic extraction mechanism of H − ions from the double-ion plasma in H − negative ion sources. The result shows the same tendency of the H − ion density n H − as that observed in the experiments, i.e., n H − in the upstream region away from the plasma meniscus (H − emitting surface) has been reduced by applying the extraction voltage. At the same time, relatively slow temporal oscillation of the electric potential compared with the electron plasma frequency has been observed in the extraction region. Results of the systematic study using a 1D3V-PIC model with the uniform magnetic field confirm the result that the electrostatic oscillation is identified to be lower hybrid wave. The effect of this oscillation on the H − transport will be studied in the future.
“…The intensity of H α emission at the far position of z = 18 mm is higher than that at close position of z = 4 owing to the electron contamination. 5 The H α signal intensity decreased 15% by beam extraction near the PG apertures. The electron temperature measured by an electrostatic probe is 2.3 eV at z = 11 mm.…”
Section: Spatial Distribution Of H α Emission In the Extraction mentioning
A spectrally selective imaging system has been developed to obtain a distribution of H α emissions at the extraction region in a hydrogen negative ion source. The diagnostic system consisted of an aspherical lens, optical filters, a fiber image conduit, and a charge coupled device detector was installed on the 1/3-scaled hydrogen negative ion source in the National Institute for Fusion Science. The center of sight line passes beside the plasma grid (PG) surface with the distance of 11 mm, and the viewing angle has coverage 35 mm from the PG surface. Two dimensional H α distribution in the range up to 20 mm from the PG surface was clearly observed. The reduction area for H α emission caused by beam extraction was widely distributed in the extraction region near the PG surface.
“…Research oriented to improvements of the negative ion source is necessary. A lot of efforts have been contributed to the improvements of negative hydrogen ion (H − ) sources, in order to increase the performance of negative ion based NBI systems [4][5][6][7][8][9][10][11][12][13] is much higher than the electron density, is generated in the beam extraction region [9]. However, the H − ion rich plasma is affected by the extraction field.…”
Experimental measurements with Langmuir probe and laser photodetachment in beam extraction region of a cesium-seeded negative ion source for NBI has been conducted in order to investigate the response of charged particles to applied external field. The profiles of probe saturation current and H − ion density in the direction normal to the plasma grid (PG) surface were measured by scanning the tip position. By comparing the results before and during beam extraction, the charged particle responses due to the beam extraction have been analyzed. During beam extraction, probe saturation current increases since H − ions are extracted and electrons flow into the extracting region for charge neutrality. The maximum increment of the probe saturation current due to electron flow appears in the range of 15 -25 mm apart from the PG surface. Meanwhile, the maximum decrement of the H − ion density is at around 18 mm from the PG. In the region far from the PG, probe saturation current increment is low as well as the decrement of the H − ion density. The extrapolations of the profiles suggest that the depth of the influence on the plasma by beam extraction is 42 mm from the plasma grid surface.
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