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Analysis of the cesium distribution in the JT-60SA negative ion sources for steady long-pulse operation.
Yoshida, M; Oohara, W; Ichikawa, M; Hiratsuka, J; Saquilayan, G Q; Umeda, N; Kojima, A; Kashiwagi, M.
Affiliation
  • Yoshida M; Division of Electrical, Electronic, and Information Engineering, Yamaguchi University, Ube 755-8611, Japan.
  • Oohara W; Division of Electrical, Electronic, and Information Engineering, Yamaguchi University, Ube 755-8611, Japan.
  • Ichikawa M; National Institutes for Quantum and Radiological Science and Technology, 801-1, Mukouyama, Naka 311-0193, Japan.
  • Hiratsuka J; National Institutes for Quantum and Radiological Science and Technology, 801-1, Mukouyama, Naka 311-0193, Japan.
  • Saquilayan GQ; National Institutes for Quantum and Radiological Science and Technology, 801-1, Mukouyama, Naka 311-0193, Japan.
  • Umeda N; National Institutes for Quantum and Radiological Science and Technology, 801-1, Mukouyama, Naka 311-0193, Japan.
  • Kojima A; National Institutes for Quantum and Radiological Science and Technology, 801-1, Mukouyama, Naka 311-0193, Japan.
  • Kashiwagi M; National Institutes for Quantum and Radiological Science and Technology, 801-1, Mukouyama, Naka 311-0193, Japan.
Rev Sci Instrum ; 91(3): 033313, 2020 Mar 01.
Article in En | MEDLINE | ID: mdl-32259933
ABSTRACT
To realize stable negative ion beams for 100 s required in the neutral beam injector of JT-60SA, a physical model to control cesium (Cs) distribution inside the negative ion source has been developed in order to maintain the stable negative ion production at the plasma grid (PG) surface with Cs. In this work, to quantitatively evaluate Cs coverage on the PG, a three-dimensional Cs transportation code was introduced to consider the spatial Cs distribution in the source. The spatial temperature distribution of the chamber wall was also introduced in this model. As a result, the reasonable variation of the Cs coverage for 100 s was obtained, compared to that in the initial model. Based on the modified model, the operational temperature of the chamber wall was proposed to be less than 60 °C to suppress the desorption of Cs in the chamber wall and to sustain the stable negative ion production. In addition, it was also suggested that a slightly higher wall temperature before the operation leads to a decrease in the amount of Cs stored at the chamber wall, resulting in suppression of Cs consumption in the ion source.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Rev Sci Instrum Year: 2020 Document type: Article Affiliation country: Japan

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Rev Sci Instrum Year: 2020 Document type: Article Affiliation country: Japan