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dc.contributor.authorJauberteau, Jean-Louises-ES
dc.contributor.authorJauberteau, Isabellees-ES
dc.contributor.authorCortázar Pérez, Osvaldo Danieles-ES
dc.contributor.authorMegia Macías, Ana Maríaes-ES
dc.date.accessioned2021-03-02T17:43:28Z
dc.date.available2021-03-02T17:43:28Z
dc.date.issued01/11/2017es_ES
dc.identifier.issn2158-3226es_ES
dc.identifier.uri10.1063/1.5001271es_ES
dc.identifier.urihttp://hdl.handle.net/11531/54714
dc.descriptionArtículos en revistases_ES
dc.description.abstractEste trabajo está dedicado al estudio de la función de distribución de energía electrónica (EEDF) durante la desintegración (afterglow) de un magnetoplasma pulsado que trabaja a 2,45 GHz en H2. Los experimentos se realizan bajo resonancia (B = 0.087T) y fuera de resonancia (B = 0.120T) condiciones, a baja (0.38Pa) y alta presión (0.62Pa) para energías entrantes que van de 300 W a 1500 W.es-ES
dc.description.abstractThiswork is devoted to the study of the Electron Energy Distribution Function (EEDF) during the decay (afterglow) of a pulsed magnetoplasma working at 2.45GHz in H2. The experiments are performed under resonance (B=0.087T) and off resonance (B=0.120T) conditions, at low(0.38Pa) and high pressure (0.62Pa) for incoming power ranging from300Wto1500W. At steady state i.e. before the discharge decay, theEEDF profile exhibits three main components of which amplitude changes under experimental conditions.Alowenergy component ("e<10eV) is observed whatever experimental conditions are. An intermediate energy component is observed at energy ranging from 5eV to 15eV under resonance conditions. A high energy component is observed up to 30eV in the EEDF tail, mainly under off resonance conditions. Standard fitting methods are used to study the change of the different EEDF components versus time during afterglow. We show that the three components stand for different times: The low and high energy component stand from 10 s to 15 s and the intermediate energy component stands for only 5 s. The different decay characteristic times are discussed and the results are correlated to the electron recombination processes in the discharge, to the reminiscent incoming power observed up to 30 s, and to the peak observed in the reflected power during decays. We show that the low energy component decay is due to the electron recombination process, which is limited by the charge transfer process which produces H3 +.en-GB
dc.format.mimetypeapplication/pdfes_ES
dc.language.isoes-ESes_ES
dc.rightsCreative Commons Reconocimiento-NoComercial-SinObraDerivada Españaes_ES
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es/es_ES
dc.sourceRevista: AIP Advances, Periodo: 1, Volumen: 7, Número: , Página inicial: 125107-1, Página final: 125107-16es_ES
dc.titleElectron energy distribution function in a pulsed 2.45GHz hydrogen magnetoplasma: Study of the decayes_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.description.versioninfo:eu-repo/semantics/publishedVersiones_ES
dc.rights.holderes_ES
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses_ES
dc.keywordsReactor de plasmaes-ES
dc.keywordsPlasma reactoren-GB


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