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Ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils

Laser-driven ion acceleration is often analyzed assuming that ionization reaches a steady state early in the interaction of the laser pulse with the target. This assumption breaks down for materials of high atomic number for which the ionization occurs concurrently with the acceleration process. Usi...

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Autores principales: Li, Jun, Arefiev, Alexey V., Bulanov, Stepan S., Kawahito, Daiki, Bailly-Grandvaux, Mathieu, Petrov, George M., McGuffey, Christopher, Beg, Farhat N.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6345865/
https://www.ncbi.nlm.nih.gov/pubmed/30679670
http://dx.doi.org/10.1038/s41598-018-37085-6
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author Li, Jun
Arefiev, Alexey V.
Bulanov, Stepan S.
Kawahito, Daiki
Bailly-Grandvaux, Mathieu
Petrov, George M.
McGuffey, Christopher
Beg, Farhat N.
author_facet Li, Jun
Arefiev, Alexey V.
Bulanov, Stepan S.
Kawahito, Daiki
Bailly-Grandvaux, Mathieu
Petrov, George M.
McGuffey, Christopher
Beg, Farhat N.
author_sort Li, Jun
collection PubMed
description Laser-driven ion acceleration is often analyzed assuming that ionization reaches a steady state early in the interaction of the laser pulse with the target. This assumption breaks down for materials of high atomic number for which the ionization occurs concurrently with the acceleration process. Using particle-in-cell simulations, we have examined acceleration and simultaneous field ionization of copper ions in ultra-thin targets (20–150 nm thick) irradiated by a laser pulse with intensity 1 × 10(21) W/cm(2). At this intensity, the laser pulse drives strong electric fields at the rear side of the target that can ionize Cu to charge states with valence L-shell or full K-shell. The highly-charged ions are produced only in a very localized region due to a significant gap between the M- and L-shells’ ionization potentials and can be accelerated by strong, forward-directed sections of the field. Such an “ionization injection” leads to well-pronounced bunches of energetic, highly-charged ions. We also find that for the thinnest target (20 nm) a push by the laser further increases the ion energy gain. Thus, the field ionization, concurrent with the acceleration, offers a promising mechanism for the production of energetic, high-charge ion bunches.
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spelling pubmed-63458652019-01-29 Ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils Li, Jun Arefiev, Alexey V. Bulanov, Stepan S. Kawahito, Daiki Bailly-Grandvaux, Mathieu Petrov, George M. McGuffey, Christopher Beg, Farhat N. Sci Rep Article Laser-driven ion acceleration is often analyzed assuming that ionization reaches a steady state early in the interaction of the laser pulse with the target. This assumption breaks down for materials of high atomic number for which the ionization occurs concurrently with the acceleration process. Using particle-in-cell simulations, we have examined acceleration and simultaneous field ionization of copper ions in ultra-thin targets (20–150 nm thick) irradiated by a laser pulse with intensity 1 × 10(21) W/cm(2). At this intensity, the laser pulse drives strong electric fields at the rear side of the target that can ionize Cu to charge states with valence L-shell or full K-shell. The highly-charged ions are produced only in a very localized region due to a significant gap between the M- and L-shells’ ionization potentials and can be accelerated by strong, forward-directed sections of the field. Such an “ionization injection” leads to well-pronounced bunches of energetic, highly-charged ions. We also find that for the thinnest target (20 nm) a push by the laser further increases the ion energy gain. Thus, the field ionization, concurrent with the acceleration, offers a promising mechanism for the production of energetic, high-charge ion bunches. Nature Publishing Group UK 2019-01-24 /pmc/articles/PMC6345865/ /pubmed/30679670 http://dx.doi.org/10.1038/s41598-018-37085-6 Text en © The Author(s) 2019 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Li, Jun
Arefiev, Alexey V.
Bulanov, Stepan S.
Kawahito, Daiki
Bailly-Grandvaux, Mathieu
Petrov, George M.
McGuffey, Christopher
Beg, Farhat N.
Ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils
title Ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils
title_full Ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils
title_fullStr Ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils
title_full_unstemmed Ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils
title_short Ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils
title_sort ionization injection of highly-charged copper ions for laser driven acceleration from ultra-thin foils
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6345865/
https://www.ncbi.nlm.nih.gov/pubmed/30679670
http://dx.doi.org/10.1038/s41598-018-37085-6
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