Role of volume and surface processes in the atomic oxygen loss frequency in oxygen glow discharges in Pyrex
| dc.bibliographicCitation.articleNumber | 085003 | |
| dc.bibliographicCitation.issue | 8 | |
| dc.bibliographicCitation.journalTitle | Plasma Sources Science and Technology | |
| dc.bibliographicCitation.volume | 34 | |
| dc.contributor.author | Viegas, Pedro | |
| dc.contributor.author | Cunha Dias, Tiago | |
| dc.contributor.author | Guerra, Vasco | |
| dc.date.accessioned | 2026-03-05T11:55:34Z | |
| dc.date.available | 2026-03-05T11:55:34Z | |
| dc.date.issued | 2025 | |
| dc.description.abstract | This work aims at understanding and finding the most accurate way to estimate an effective O surface recombination probability ( γ O ) from the temporal evolution of O(<sup>3</sup>P) density measured in modulated current conditions in the positive column of oxygen glow discharges in Pyrex, which is relevant for experimental characterization and for model inputs. The procedure for deducing γ O from the O loss frequency ( ν O loss ) is not straightforward, since the processes determining the net losses of O(<sup>3</sup>P) are not known a priori. A global model describing plasma chemical kinetics is used in steady-state and current-modulated modes to assess the physical meaning of ν O loss , for a total of 66 experimental conditions in the pressure range 0.4-7.5 Torr with 7.8 sccm flow rate and 20-40 mA currents. An optimal γ O is derived from ν O loss and the accuracy of different hypotheses on the relevant processes for the net losses of O(<sup>3</sup>P) is addressed. The hypothesis that is found to be the most accurate indicates that the net loss of O(<sup>3</sup>P) is due not only to surface recombination, but also to recombination in volume and to flow losses. Volume processes account on average for 24% of O(<sup>3</sup>P) net losses, and that fraction tendentiously grows with pressure, reaching up to 71%. The verified hypothesis can be adopted for the estimation of γ O from the measured ν O loss in both discharge (partial modulation) and post-discharge (full modulation) conditions. Finally, a discussion is had on what steps can be taken for a complete validation of the oxygen glow discharge model. | eng |
| dc.description.version | publishedVersion | eng |
| dc.identifier.uri | https://oa.tib.eu/renate/handle/123456789/32045 | |
| dc.identifier.uri | https://doi.org/10.34657/31114 | |
| dc.language.iso | eng | |
| dc.publisher | Bristol : IOP Publ. | |
| dc.relation.doi | https://doi.org/10.1088/1361-6595/adf5e4 | |
| dc.relation.essn | 1361-6595 | |
| dc.relation.issn | 0963-0252 | |
| dc.rights.license | CC BY 4.0 Unported | |
| dc.rights.uri | https://creativecommons.org/licenses/by/4.0 | |
| dc.subject.ddc | 530 | |
| dc.subject.other | global model | eng |
| dc.subject.other | oxygen kinetics | eng |
| dc.subject.other | recombination probability | eng |
| dc.subject.other | surface recombination | eng |
| dc.subject.other | LTP research | eng |
| dc.title | Role of volume and surface processes in the atomic oxygen loss frequency in oxygen glow discharges in Pyrex | eng |
| dc.type | Article | |
| tib.accessRights | openAccess |
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