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rf plasma source using a magnetic line‐cusp field
A large volume cylindrical radio frequency (rf) plasma source using a magnetic line‐cusp field has been developed for use in large scale plasma processing. In this type of plasma source, a capacitively coupled 13.56 MHz rf plasma is produced in the presence of a magnetic line‐cusp field. Three versi...
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Published in: | Review of scientific instruments 1993-09, Vol.64 (9), p.2434-2439 |
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Language: | English |
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container_end_page | 2439 |
container_issue | 9 |
container_start_page | 2434 |
container_title | Review of scientific instruments |
container_volume | 64 |
creator | Yamauchi, Kazuo Takahashi, Keiji Yabe, Eiji |
description | A large volume cylindrical radio frequency (rf) plasma source using a magnetic line‐cusp field has been developed for use in large scale plasma processing. In this type of plasma source, a capacitively coupled 13.56 MHz rf plasma is produced in the presence of a magnetic line‐cusp field. Three versions of the plasma source have been constructed and tested. The first version has a pair of peripheral rf electrodes placed outside the ionization chamber and is suitable for preparing a large volume uniform plasma. This plasma source can attain a useful area of plasma with 10% uniformity over a 30‐cm‐diam region. The second version is featured by parallel doughnut‐plate electrodes which form part of the chamber wall and serve as a high current source, where the electron density is proportional to the rf power, being equal to 4×1010 cm−3 at 400 W. The third version is a slab‐plasma source, which has a rectangular ionization chamber, a pair of rectangular magnetic coils, and a pair of rectangular rf electrodes, yielding an electron density of the order of 109 cm−3 for a 25 W rf power. |
doi_str_mv | 10.1063/1.1143901 |
format | article |
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In this type of plasma source, a capacitively coupled 13.56 MHz rf plasma is produced in the presence of a magnetic line‐cusp field. Three versions of the plasma source have been constructed and tested. The first version has a pair of peripheral rf electrodes placed outside the ionization chamber and is suitable for preparing a large volume uniform plasma. This plasma source can attain a useful area of plasma with 10% uniformity over a 30‐cm‐diam region. The second version is featured by parallel doughnut‐plate electrodes which form part of the chamber wall and serve as a high current source, where the electron density is proportional to the rf power, being equal to 4×1010 cm−3 at 400 W. 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In this type of plasma source, a capacitively coupled 13.56 MHz rf plasma is produced in the presence of a magnetic line‐cusp field. Three versions of the plasma source have been constructed and tested. The first version has a pair of peripheral rf electrodes placed outside the ionization chamber and is suitable for preparing a large volume uniform plasma. This plasma source can attain a useful area of plasma with 10% uniformity over a 30‐cm‐diam region. The second version is featured by parallel doughnut‐plate electrodes which form part of the chamber wall and serve as a high current source, where the electron density is proportional to the rf power, being equal to 4×1010 cm−3 at 400 W. The third version is a slab‐plasma source, which has a rectangular ionization chamber, a pair of rectangular magnetic coils, and a pair of rectangular rf electrodes, yielding an electron density of the order of 109 cm−3 for a 25 W rf power.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.1143901</doi><tpages>6</tpages></addata></record> |
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identifier | ISSN: 0034-6748 |
ispartof | Review of scientific instruments, 1993-09, Vol.64 (9), p.2434-2439 |
issn | 0034-6748 1089-7623 |
language | eng |
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source | AIP_美国物理联合会现刊(与NSTL共建); AIP Digital Archive |
subjects | Exact sciences and technology Physics Physics of gases, plasmas and electric discharges Physics of plasmas and electric discharges Plasma production and heating Plasma sources |
title | rf plasma source using a magnetic line‐cusp field |
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