<p>The behavior of mixed composition cold non-equilibrium plasmas was investigated in a low-pressure capacitively coupled reactor using optical emission spectroscopy (OES). By fitting experimental data to simulations of the Second Positive System (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\:{C\:}^{3}{{\Pi\:}}_{u}-{B\:}^{3}{{\Pi\:}}_{g}\)</EquationSource> </InlineEquation>) of N<sub>2</sub>, rotational and vibrational temperatures were determined for various Ar/N<sub>2</sub> mixtures as a function of plasma input power (40–100&#xa0;W) and pressure (300–700 mTorr). Simulations of the plasma were performed for comparison. For pure N<sub>2</sub>, the observed trends revealed that both the rotational and vibrational temperatures increased with input power, (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\:{T}_{rot}\)</EquationSource> </InlineEquation> of <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\:v=0\)</EquationSource> </InlineEquation> increased from 369 to 396&#xa0;K and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\:{T}_{vib\:}\)</EquationSource> </InlineEquation> from 5938 to 6542&#xa0;K, at 40–100&#xa0;W, 100 SCCM and 293 mTorr) but both temperatures showed minimal response to the applied changes in pressure. The rotational and vibrational temperatures for the mixed composition Ar/N<sub>2</sub> plasmas were significantly higher compared to the pure N<sub>2</sub> plasmas (e.g. <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\:{T}_{rot}\)</EquationSource> </InlineEquation> of 1308&#xa0;K and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\:{T}_{vib}\)</EquationSource> </InlineEquation> of 7279&#xa0;K for 1.8% of N<sub>2</sub> in Ar; at 50&#xa0;W, 4 SCCM of N<sub>2</sub>, 220 SCCM of Ar for a total pressure of 587 mTorr). Moreover, the addition of Ar caused a larger separation between the rotational and vibrational temperatures compared to the pure N<sub>2</sub> case. These phenomena illustrate the effects of Ar on the non-equilibrium energy distribution and more generally the influence that the gas mixture composition may have on the plasma reactivity.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Analysis of Mixed Composition Cold Plasmas by Optical Emission Diagnostics and Simulations

  • Shani Har Lavan,
  • Sharona Atlas,
  • Amir Kaplan,
  • Avi Lehrer,
  • Illya Rozenberg,
  • Hao Zhao,
  • Joshua H. Baraban

摘要

The behavior of mixed composition cold non-equilibrium plasmas was investigated in a low-pressure capacitively coupled reactor using optical emission spectroscopy (OES). By fitting experimental data to simulations of the Second Positive System ( \(\:{C\:}^{3}{{\Pi\:}}_{u}-{B\:}^{3}{{\Pi\:}}_{g}\) ) of N2, rotational and vibrational temperatures were determined for various Ar/N2 mixtures as a function of plasma input power (40–100 W) and pressure (300–700 mTorr). Simulations of the plasma were performed for comparison. For pure N2, the observed trends revealed that both the rotational and vibrational temperatures increased with input power, ( \(\:{T}_{rot}\) of \(\:v=0\) increased from 369 to 396 K and \(\:{T}_{vib\:}\) from 5938 to 6542 K, at 40–100 W, 100 SCCM and 293 mTorr) but both temperatures showed minimal response to the applied changes in pressure. The rotational and vibrational temperatures for the mixed composition Ar/N2 plasmas were significantly higher compared to the pure N2 plasmas (e.g. \(\:{T}_{rot}\) of 1308 K and \(\:{T}_{vib}\) of 7279 K for 1.8% of N2 in Ar; at 50 W, 4 SCCM of N2, 220 SCCM of Ar for a total pressure of 587 mTorr). Moreover, the addition of Ar caused a larger separation between the rotational and vibrational temperatures compared to the pure N2 case. These phenomena illustrate the effects of Ar on the non-equilibrium energy distribution and more generally the influence that the gas mixture composition may have on the plasma reactivity.