Broad ion energy distributions in helicon wave-coupled helium plasma

Helium ion energy distributions were measured in helicon wave-coupled plasmas of the dynamics of ion implantation and sputtering of surface experiment using a retarding field energy analyzer. The shape of the energy distribution is a double-peak, characteristic of radiofrequency plasma potential mod...

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Bibliographic Details
Main Authors: Woller, Kevin Benjamin (Contributor), Whyte, Dennis G (Contributor), Wright, Graham (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Nuclear Science and Engineering (Contributor), Massachusetts Institute of Technology. Plasma Science and Fusion Center (Contributor)
Format: Article
Language:English
Published: American Institute of Physics (AIP), 2018-07-25T18:47:58Z.
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Online Access:Get fulltext
LEADER 02170 am a22002413u 4500
001 117126
042 |a dc 
100 1 0 |a Woller, Kevin Benjamin  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Nuclear Science and Engineering  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Plasma Science and Fusion Center  |e contributor 
100 1 0 |a Woller, Kevin Benjamin  |e contributor 
100 1 0 |a Whyte, Dennis G  |e contributor 
100 1 0 |a Wright, Graham  |e contributor 
700 1 0 |a Whyte, Dennis G  |e author 
700 1 0 |a Wright, Graham  |e author 
245 0 0 |a Broad ion energy distributions in helicon wave-coupled helium plasma 
260 |b American Institute of Physics (AIP),   |c 2018-07-25T18:47:58Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/117126 
520 |a Helium ion energy distributions were measured in helicon wave-coupled plasmas of the dynamics of ion implantation and sputtering of surface experiment using a retarding field energy analyzer. The shape of the energy distribution is a double-peak, characteristic of radiofrequency plasma potential modulation. The broad distribution is located within a radius of 0.8 cm, while the quartz tube of the plasma source has an inner radius of 2.2 cm. The ion energy distribution rapidly changes from a double-peak to a single peak in the radius range of 0.7-0.9 cm. The average ion energy is approximately uniform across the plasma column including the double-peak and single peak regions. The widths of the broad distribution, ΔE, in the wave-coupled mode are large compared to the time-averaged ion energy, 〈E〉. On the axis (r = 0), ΔE/ 〈E〉 ≲ 3.4, and at a radius near the edge of the plasma column (r = 2.2 cm), ΔE/ 〈E〉 ∼ 1.2. The discharge parameter space is scanned to investigate the effects of the magnetic field, input power, and chamber fill pressure on the wave-coupled mode that exhibits the sharp radial variation in the ion energy distribution. 
520 |a United States. Department of Energy (Award DESC00-02060) 
520 |a United States. Department of Energy (Award DE-FC02-99ER54512) 
655 7 |a Article 
773 |t Physics of Plasmas