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2D hybrid simulation of a dual-frequency capacitively coupled nitrogen discharge: effects of gas pressure and low-frequency voltage on generation and distribution of species
The effect of the gas pressure and the low frequency voltage, V LF , on the spatial distributions of electron energy distribution function (EEDF), electron and neutral densities in a dual-frequency (DF 2/60 MHz) driven capacitive discharge in nitrogen (N 2 ) is investigated by employing a two-dimens...
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Published in: | Journal of physics. D, Applied physics Applied physics, 2025-03, Vol.58 (12), p.125201 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | The effect of the gas pressure and the low frequency voltage, V LF , on the spatial distributions of electron energy distribution function (EEDF), electron and neutral densities in a dual-frequency (DF 2/60 MHz) driven capacitive discharge in nitrogen (N 2 ) is investigated by employing a two-dimensional fluid model with electron collision processes treated by Monte Carlo model. It is found that by increasing the pressure the region of strong ionization shrinks immensely towards the sheath edge of the powered electrode and the ionization maximum occurs below the edge of the powered electrode, leading to edge-high density profiles of the electron and excited-state nitrogen molecules at a higher pressure, while the nitrogen atom density remains uniform in space, due to higher transport coefficient. By increasing V LF , the discharge becomes more symmetrical in axial direction, the ionization rate changes from a radial uniform to an edge-high profile, leading to an edge-high profile of electron density. The EEDF is found to exhibit a dip at ε = 2.35 eV, due to depletion of electron via the electron-impact vibrational excitation of nitrogen molecule. This dip of the EEDF is most significant at the discharge center, and become less pronounced towards the sheath edge and the sidewall, due to low-energy electrons being heated by local strong electric field. Besides, at a higher V LF , the dip becomes less significant, due to enhanced electron heating. |
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ISSN: | 0022-3727 1361-6463 |
DOI: | 10.1088/1361-6463/ada6c0 |