PHYSICS OF GASES, PLASMAS, AND ELECTRIC DISCHARGES |
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Exploration of the Townsend regime by discharge light emission in a gas discharge device |
Hilal Yucel Kurt |
Gazi University, Faculty of Sciences, Department of Physics, 06500 Ankara, Turkey |
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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.
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Received: 08 March 2013
Revised: 18 April 2013
Accepted manuscript online:
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PACS:
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52.80.Dy
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(Low-field and Townsend discharges)
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52.77.-j
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(Plasma applications)
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73.61.Ey
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(III-V semiconductors)
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Fund: Project supported by Gazi University BAP Research Project, Turkey (Grant Nos. 05/2012-47 and 05/2012-72). |
Corresponding Authors:
Hilal Yucel Kurt
E-mail: hyucelkurt@gmail.com
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Cite this article:
Hilal Yucel Kurt Exploration of the Townsend regime by discharge light emission in a gas discharge device 2014 Chin. Phys. B 23 015201
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