We discuss a technique for using an emissive probe to measure accurately the time‐invariant plasma potential in a rf generated plasma, usually used in plasma processing. With an emissive probe, a short length of filament, heated to thermionic emission, is immersed in the plasma. We have introduced into each lead of the filament two LC circuits, one resonant at 13.6 MHz, the fundamental rf frequency, and the other at 27.2 MHz, the first harmonic. With the LC circuits in place a single peak of di/dv versus v occurs with a maximum at the time‐invariant plasma potential. The inflection point method of measuring this potential described by Smith, Hershkowitz, and Coakley [Rev. Sci. Instrum. 50, 210 (1979)] in a dc plasma is now operative. The estimated error in measuring this potential is ±3.5%.
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Research Article|
May 01 1996
A radio frequency compensated emissive probe
Jungwon Kang;
Jungwon Kang
Department of Electrical and Computer Engineering, University of Arizona, Tucson, Arizona 85721
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Robert N. Carlile;
Robert N. Carlile
Department of Electrical and Computer Engineering, University of Arizona, Tucson, Arizona 85721
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John F. O’Hanlon
John F. O’Hanlon
Department of Electrical and Computer Engineering, University of Arizona, Tucson, Arizona 85721
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Rev. Sci. Instrum. 67, 1818–1821 (1996)
Article history
Received:
November 20 1995
Accepted:
January 16 1996
Citation
Jungwon Kang, Robert N. Carlile, John F. O’Hanlon; A radio frequency compensated emissive probe. Rev. Sci. Instrum. 1 May 1996; 67 (5): 1818–1821. https://doi.org/10.1063/1.1146980
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