2009
DOI: 10.1088/0963-0252/18/4/045021
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On the formation mechanisms of the diffuse atmospheric pressure dielectric barrier discharge in CVD processes of thin silica-like films

Abstract: Pathways of formation and temporal evolution of the diffuse dielectric barrier discharge at atmospheric pressure were experimentally studied in this work by means of optical (fast imaging camera) and electrical diagnostics. The chosen model system is relevant for applications of plasma-enhanced chemical vapor deposition of thin silica-like film on the polymeric substrate, from cost-efficient gas mixtures of Ar/N 2 /O 2 /hexamethyldisiloxane. It was found that the discharge can gradually experience the phases o… Show more

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Cited by 62 publications
(75 citation statements)
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References 28 publications
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“…Alternatively, stability is achieved by coating at least one electrode with an insulating layer and applying an AC potential. Once the discharge is initiated, surface charging of the insulator limits the electric field inside the plasma, extinguishing the ionization rate within a microsecond or less [24][25][26][27][28] The duration of the discharge is less than the IOI time constant. The dielectric barrier discharge (DBD) is quite widely used due to this simple and effective stabilization of the IOI.…”
Section: Introductionmentioning
confidence: 99%
“…Alternatively, stability is achieved by coating at least one electrode with an insulating layer and applying an AC potential. Once the discharge is initiated, surface charging of the insulator limits the electric field inside the plasma, extinguishing the ionization rate within a microsecond or less [24][25][26][27][28] The duration of the discharge is less than the IOI time constant. The dielectric barrier discharge (DBD) is quite widely used due to this simple and effective stabilization of the IOI.…”
Section: Introductionmentioning
confidence: 99%
“…The emission intensity therefore indicate the information of the high-energy electrons in the tail of the EEDF (13.5 eV and 13.3 eV in this study). From figure 5, the LF discharge (P LF = 120 W) can be characterized as operating in 'glow-like' mode with maximal emission intensity close to the electrodes, as previously studied in [11] using nitrogen/oxygen gas mixtures. The RF discharge mode depends on the amplitude of the input power.…”
Section: Time-integrated Plasma Emissionmentioning
confidence: 60%
“…The characteristic transverse excitation intensity profiles corresponding to phase (1) and (2) in figure 6 are presented in figure 7. As previously studied by Starostin et al for similar conditions in an N 2 /O 2 gas mixture, the LF discharge is initiated by the Townsend breakdown mechanism [11]. The space charge produced from the preceding half cycle would affect the electric field and reduce the breakdown voltage at the ignition of the next discharge.…”
Section: Phase-resolved Electron Impact Excitationmentioning
confidence: 83%
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“…In this study, the gas loss is estimated at about 30%. 25 In the deposition, the tetraethylorthosilicate (TEOS) precursor was diluted with 1.0 slm argon together with oxygen as the oxidizer and 15 slm nitrogen as the carrier gas. The DBD was powered by a sinusoidal voltage with a frequency of 185 kHz and amplitude up to 2-3 kV.…”
Section: Experimental Set-upmentioning
confidence: 99%