Spatial distribution of the charged particles and potentials during beam extraction in a negative-ion source

  • K. Tsumori
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • H. Nakano
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • M. Kisaki
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • K. Ikeda
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • K. Nagaoka
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • M. Osakabe
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • Y. Takeiri
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • O. Kaneko
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • M. Shibuya
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • E. Asano
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • T. Kondo
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • M. Sato
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • S. Komada
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • H. Sekiguchi
    National Institute for Fusion Science 1 , 322-1 Oroshi Toki-city, Figu 509-5292, Japan
  • N. Kameyama
    Keio University 2 , 3-14-1 Hiyoshi, Kouhoku-ku, Yokohama 223-8522, Japan
  • T. Fukuyama
    Keio University 2 , 3-14-1 Hiyoshi, Kouhoku-ku, Yokohama 223-8522, Japan
  • S. Wada
    Keio University 2 , 3-14-1 Hiyoshi, Kouhoku-ku, Yokohama 223-8522, Japan
  • A. Hatayama
    Keio University 2 , 3-14-1 Hiyoshi, Kouhoku-ku, Yokohama 223-8522, Japan

Abstract

<jats:p>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 extraction and the electron density jumps up correspondingly. The time integral of the decreasing H− charge density agrees well with the electron charge collected with the probe. The agreement of the charges is interpreted to indicate that the H− density decreasing at the beam extraction is compensated by the electrons diffusing from the driver region. In the plasmas with very low electron density, the pre-sheath of the extraction field penetrates deeply inside the plasmas. That is because the shielding length in those plasmas is longer than that in the usual electron-ion plasmas, and furthermore the electrons are suppressed to diffuse to the extraction region due to the strong magnetic field.</jats:p>

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