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ORCID: https://orcid.org/0000-0002-7460-6561, Colón Hernández, Cristóbal
ORCID: https://orcid.org/0000-0003-4663-7122, Porro González, Juan Antonio
ORCID: https://orcid.org/0000-0001-5260-527X and Ocaña Moreno, José Luis
ORCID: https://orcid.org/0000-0001-9263-8404
(2016).
Measurement of plasma electron density generated in an experiment of laser shock processing, utilizing the Hα-line.
"Journal of Materials Processing Technology", v. 232
;
pp. 9-18.
ISSN 0924-0136.
https://doi.org/10.1016/j.jmatprotec.2016.01.026.
| Título: | Measurement of plasma electron density generated in an experiment of laser shock processing, utilizing the Hα-line |
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| Autor/es: |
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| Tipo de Documento: | Artículo |
| Título de Revista/Publicación: | Journal of Materials Processing Technology |
| Fecha: | Junio 2016 |
| ISSN: | 0924-0136 |
| Volumen: | 232 |
| Materias: | |
| ODS: | |
| Palabras Clave Informales: | Laser shock processing; plasma diagnosis; electron density; Hydrogen |
| Escuela: | E.T.S.I. Diseño Industrial (UPM) |
| Departamento: | Ingeniería Eléctrica, Electrónica Automática y Física Aplicada |
| Licencias Creative Commons: | Reconocimiento - Sin obra derivada - No comercial |
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In this work we have realized plasma diagnosis produced by Laser (LPP), by means of emission spectroscopy in a Laser Shock Processing (LSP). The LSP has been proposed as an alternative technology, competitive with classical surface treatments. The ionic species present in the plasma together with electron density and its temperature provide significant indicators of the degree of surface effect of the treated material. In order to analyze these indicators, we have realized spectroscopic studies of optical emission in the laser-generated plasmas in different situations. We have worked focusing on an aluminum sample (Al2024) in air and/or in LSP conditions (water flow) a Q-switched laser of Nd:YAG (λ = 1.06 μm, 10 ns of pulse duration, running at 10 Hz repetition rate). The pulse energy was set at 2,5 J per pulse. The electron density has been measured using, in every case, the Stark broadening of H Balmer α line (656.27 nm). In the case of the air, this measure has been contrasted with the value obtained with the line of 281.62 nm of Al II. Special attention has been paid to the self-absorption of the spectral lines used. The measures were realized with different delay times after the pulse of the laser (1–8 μs) and with a time window of 1 μs. In LSP the electron density obtained was between 1017 cm−3 for the shortest delays (4–6 μs), and 1016 cm−3 for the greatest delays (7,8 μs).
| ID de Registro: | 39474 |
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| Identificador DC: | https://oa.upm.es/39474/ |
| Identificador OAI: | oai:oa.upm.es:39474 |
| URL Portal Científico: | https://portalcientifico.upm.es/es/ipublic/item/5493599 |
| Identificador DOI: | 10.1016/j.jmatprotec.2016.01.026 |
| URL Oficial: | https://doi.org/10.1016/j.jmatprotec.2016.01.026 |
| Depositado por: | Memoria Investigacion |
| Depositado el: | 26 Feb 2016 09:48 |
| Ultima Modificación: | 12 Nov 2025 00:00 |
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