2021
DOI: 10.1103/physreve.104.045209
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Resonant sheath heating in weakly magnetized capacitively coupled plasmas due to electron-cyclotron motion

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Cited by 31 publications
(28 citation statements)
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“…Recently, a new operational regime is identified in low-pressure very high frequency (VHF) CCP discharge in the presence of a weak uniform external magnetic field. It is shown that high plasma density and thereby high ion flux can be achieved even at a very weak external magnetic field (~ 10 G) where ion energy can also be optimized simultaneously [34][35][36][37][38]. It is also reported in the literature that using magnetic field asymmetry in single-frequency CCP can independently control the ion flux and ion energy [39][40].…”
Section: Introductionmentioning
confidence: 96%
“…Recently, a new operational regime is identified in low-pressure very high frequency (VHF) CCP discharge in the presence of a weak uniform external magnetic field. It is shown that high plasma density and thereby high ion flux can be achieved even at a very weak external magnetic field (~ 10 G) where ion energy can also be optimized simultaneously [34][35][36][37][38]. It is also reported in the literature that using magnetic field asymmetry in single-frequency CCP can independently control the ion flux and ion energy [39][40].…”
Section: Introductionmentioning
confidence: 96%
“…[23] Very recently, Zhang et al revealed another similar resonance heating effect in a weakly magnetized CCP at low pressure. [24] If half of the electron cyclotron period coincides with the RF period, electrons will coherently collide with the expanding sheath and gain substantial energy via each interaction, which significantly enhances the plasma density. The dynamics can be revealed in Fig.…”
Section: Electron Heatingmentioning
confidence: 99%
“…Another electron heating mechanism related to the magnetic field and based on the resonance between the sheath motion and the Larmor rotation leading to the condition ω = 2 ω ce was investigated in [25] and named there "electron sheath resonance". Recently, it has been revisited in a number of papers [26,27,28], where it acquired a new name "electron bounce-cyclotron resonance heating". This effect, however, requires rather weak magnetic fields (e.g., for the driving frequency of 13.56 MHz studied in the present work the resonance condition leads to B = 0.24 mT).…”
Section: Introductionmentioning
confidence: 99%