2022
DOI: 10.1063/5.0087182
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Experimental study on the ignition process of a pulsed capacitively coupled RF discharge: Effects of gas pressure and voltage amplitude

Abstract: The effects of gas pressure and voltage amplitude on the ignition process of a pulse capacitively coupled RF argon discharge are experimentally investigated. The electron density is measured by a hairpin probe, the spatiotemporal distribution of the electron impact excitation dynamics is determined by phase resolved optical emission spectroscopy, and the electrical parameters are obtained by analyzing the measured current and voltage waveforms. In this work, the pulse plasma is ignited with few initial electro… Show more

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Cited by 7 publications
(4 citation statements)
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“…Particularly, the maximum of the OEI upon the overshoot becomes higher than that of P rf , provided that the scales of two vertical axes are adjusted such that the OEI and P rf curves are overlapped at p = 30 pa. This is because, as Wang et al explained in [54], the electron energy during the ignition phase is mainly dissipated via excitation collision since the pressure is relatively high and electrons are more likely to reach the threshold energies of excitation (13.5 eV). As time advances, in all the pressures investigated here, P rf increases after the ignition phase with a larger growth rate than the OEI, and the reason is given as follows.…”
Section: Pressure Effectmentioning
confidence: 99%
“…Particularly, the maximum of the OEI upon the overshoot becomes higher than that of P rf , provided that the scales of two vertical axes are adjusted such that the OEI and P rf curves are overlapped at p = 30 pa. This is because, as Wang et al explained in [54], the electron energy during the ignition phase is mainly dissipated via excitation collision since the pressure is relatively high and electrons are more likely to reach the threshold energies of excitation (13.5 eV). As time advances, in all the pressures investigated here, P rf increases after the ignition phase with a larger growth rate than the OEI, and the reason is given as follows.…”
Section: Pressure Effectmentioning
confidence: 99%
“…Figure 3(f) displays the corresponding computed values of P H and P L and the total electron impact excitation rate, K ex , as well as the computed electron and ion density, n e and n i , at the discharge center. Similar to previous works [27,28,43], the plasma ignition process is analyzed by dividing this period into three phases (see figure 3). The blue, yellow, and pink parts indicate the pre-ignition (0 ⩽ t/T L ⩽ t 1 ), ignition (t 1 ⩽ t/T L ⩽ t 2 ), and post-ignition phases (t/T L ⩾ t 2 ), respectively.…”
Section: Base Case (Vmentioning
confidence: 99%
“…Pure argon gas of a fixed flow rate of 6 sccm is introduced into the chamber, and the gas pressure is kept at 450 mTorr, of which the value is intentionally kept the same as that in our previous work [25,26]. The reason is that 450 mTorr is an intermediate pressure within the 'drift-diffusion' branch of the breakdown curve, and within the corresponding pressure range electron multiplication is primarily dominated by volume processes during plasma ignition [29].…”
Section: Experimental Setup and Diagnosticsmentioning
confidence: 99%