Chin. Phys. B ›› 2014, Vol. 23 ›› Issue (1): 15201-015201.doi: 10.1088/1674-1056/23/1/015201

• PHYSICS OF GASES, PLASMAS, AND ELECTRIC DISCHARGES • 上一篇    下一篇

Exploration of the Townsend regime by discharge light emission in a gas discharge device

Hilal Yucel Kurt   

  1. Gazi University, Faculty of Sciences, Department of Physics, 06500 Ankara, Turkey
  • 收稿日期:2013-03-08 修回日期:2013-04-18 出版日期:2013-11-12 发布日期:2013-11-12
  • 基金资助:
    Project supported by Gazi University BAP Research Project, Turkey (Grant Nos. 05/2012-47 and 05/2012-72).

Exploration of the Townsend regime by discharge light emission in a gas discharge device

Hilal Yucel Kurt   

  1. Gazi University, Faculty of Sciences, Department of Physics, 06500 Ankara, Turkey
  • Received:2013-03-08 Revised:2013-04-18 Online:2013-11-12 Published:2013-11-12
  • Contact: Hilal Yucel Kurt E-mail:hyucelkurt@gmail.com
  • Supported by:
    Project supported by Gazi University BAP Research Project, Turkey (Grant Nos. 05/2012-47 and 05/2012-72).

摘要: The Townsend discharge mechanism has been explored in a planar microelectronic gas discharge device (MGDD) with different applied voltages U and interelectrode distance d under various pressures in air. The anode and the cathode of the MGDD are formed by a transparent SnO2 covered glass and a GaAs semiconductor, respectively. In the experiments, the discharge is found to be unstable just below the breakdown voltage Ub, whereas the discharge passes through a homogeneous stable Townsend mode beyond the breakdown voltage. The measurements are made by an electrical circuit and a CCD camera by recording the currents and light emission (LE) intensities. The intensity profiles, which are converted from the 3D light emission images along the semiconductor diameter, have been analysed for different system parameters. Different instantaneous conductivity σt regimes are found below and beyond the Townsend region. These regimes govern the current and spatio-temporal LE stabilities in the plasma system. It has been proven that the stable LE region increases up to 550 Torr as a function of pressure for small d. If the active area of the semiconductor becomes larger and the interlectrode distance d becomes smaller, the stable LE region stays nearly constant with pressure.

关键词: Townsend discharge, breakdown, microelectronic gas discharge device, semiconductor cathode

Abstract: The Townsend discharge mechanism has been explored in a planar microelectronic gas discharge device (MGDD) with different applied voltages U and interelectrode distance d under various pressures in air. The anode and the cathode of the MGDD are formed by a transparent SnO2 covered glass and a GaAs semiconductor, respectively. In the experiments, the discharge is found to be unstable just below the breakdown voltage Ub, whereas the discharge passes through a homogeneous stable Townsend mode beyond the breakdown voltage. The measurements are made by an electrical circuit and a CCD camera by recording the currents and light emission (LE) intensities. The intensity profiles, which are converted from the 3D light emission images along the semiconductor diameter, have been analysed for different system parameters. Different instantaneous conductivity σt regimes are found below and beyond the Townsend region. These regimes govern the current and spatio-temporal LE stabilities in the plasma system. It has been proven that the stable LE region increases up to 550 Torr as a function of pressure for small d. If the active area of the semiconductor becomes larger and the interlectrode distance d becomes smaller, the stable LE region stays nearly constant with pressure.

Key words: Townsend discharge, breakdown, microelectronic gas discharge device, semiconductor cathode

中图分类号:  (Low-field and Townsend discharges)

  • 52.80.Dy
52.77.-j (Plasma applications) 73.61.Ey (III-V semiconductors)