4.6 Article

Spatial emission distribution of a pulsed radiofrequency glow discharge: Influence of the pulse frequency

Journal

SPECTROCHIMICA ACTA PART B-ATOMIC SPECTROSCOPY
Volume 68, Issue -, Pages 24-33

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.sab.2012.01.008

Keywords

Pulsed radiofrequency GD; Spatial resolution; Optical emission

Categories

Funding

  1. EU through the Marie Curie Research Training Network GLADNET [MRTN-CT-2006-035459]
  2. STREP [STRP 032202]
  3. Spanish Ministry of Science and Innovation
  4. FEDER [MAT2007-65097-C02, MAT2010-20921-C02]
  5. Spanish Ministry of Education
  6. European Social Fund

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A pulsed radiofrequency Glow Discharge (pulsed rf GD) plasma has been spectroscopically characterized by performing side-on measurements of the emitted radiation. The effect of varying the pulse frequency (e.g. between 100 and 10,000 Hz), while keeping the duty cycle constant at 25%, has been investigated on different argon and analyte (i.e. copper) emission lines, at different plasma locations. In particular, it is observed that an intermediate frequency of 2.5 kHz favors the excitation of the argon atoms, while the argon ions are preferably excited by lower frequencies (e.g. longer pulse widths). Moreover, the excitation of copper atoms has a strong dependence on the upper energy level, and it has been noticed that the emission from higher levels is favored by the use of lower pulsed-rf frequencies. On the other hand, it has been found that the spatial distribution of the gas species and the analyte species (i.e. Ar and Cu, respectively) differ from each other: the atomic argon emission extends longer along the plasma plume than the atomic copper emission. Furthermore, ionic species have their maximum emission signal in the region close to the anode; however, their emission signal decay quite fast at increasing distances to the anode. Nevertheless, it should be highlighted that it is possible to detect ionic emission at distances far away from the negative glow; in regions where usually the sampler cone interface is placed in GD-MS instruments. (C) 2012 Elsevier B.V. All rights reserved.

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