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Impact of the pulse contrast ratio on molybdenum K(α) generation by ultrahigh intensity femtosecond laser solid interaction
We present an extended experimental study of the absolute yield of K(α) x-ray source (17.48 keV) produced by interaction of an ultrahigh intensity femtosecond laser with solid Mo target for temporal contrast ratios in the range of 1.7 × 10(7)–3.3 × 10(9) and on three decades of intensity 10(16)–10(1...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2018
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5841281/ https://www.ncbi.nlm.nih.gov/pubmed/29515179 http://dx.doi.org/10.1038/s41598-018-22487-3 |
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author | Azamoum, Y. Tcheremiskine, V. Clady, R. Ferré, A. Charmasson, L. Utéza, O. Sentis, M. |
author_facet | Azamoum, Y. Tcheremiskine, V. Clady, R. Ferré, A. Charmasson, L. Utéza, O. Sentis, M. |
author_sort | Azamoum, Y. |
collection | PubMed |
description | We present an extended experimental study of the absolute yield of K(α) x-ray source (17.48 keV) produced by interaction of an ultrahigh intensity femtosecond laser with solid Mo target for temporal contrast ratios in the range of 1.7 × 10(7)–3.3 × 10(9) and on three decades of intensity 10(16)–10(19) W/cm². We demonstrate that for intensity I ≥ 2 × 10(18) W/cm² K(α) x-ray emission is independent of the value of contrast ratio. In addition, no saturation of the K(α) photon number is measured and a value of ~2 × 10(10) photons/sr/s is obtained at 10 Hz and I ~10(19) W/cm². Furthermore, K(α) energy conversion efficiency reaches the same high plateau equal to ~2 × 10(−4) at I = 10(19) W/cm² for all the studied contrast ratios. This original result suggests that relativistic J × B heating becomes dominant in these operating conditions which is supposed to be insensitive to the electron density gradient scale length L/λ. Finally, an additional experimental study performed by changing the angle of incidence of the laser beam onto the solid target highlights a clear signature of the interplay between collisionless absorption mechanisms depending on the contrast ratio and intensity. |
format | Online Article Text |
id | pubmed-5841281 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2018 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-58412812018-03-13 Impact of the pulse contrast ratio on molybdenum K(α) generation by ultrahigh intensity femtosecond laser solid interaction Azamoum, Y. Tcheremiskine, V. Clady, R. Ferré, A. Charmasson, L. Utéza, O. Sentis, M. Sci Rep Article We present an extended experimental study of the absolute yield of K(α) x-ray source (17.48 keV) produced by interaction of an ultrahigh intensity femtosecond laser with solid Mo target for temporal contrast ratios in the range of 1.7 × 10(7)–3.3 × 10(9) and on three decades of intensity 10(16)–10(19) W/cm². We demonstrate that for intensity I ≥ 2 × 10(18) W/cm² K(α) x-ray emission is independent of the value of contrast ratio. In addition, no saturation of the K(α) photon number is measured and a value of ~2 × 10(10) photons/sr/s is obtained at 10 Hz and I ~10(19) W/cm². Furthermore, K(α) energy conversion efficiency reaches the same high plateau equal to ~2 × 10(−4) at I = 10(19) W/cm² for all the studied contrast ratios. This original result suggests that relativistic J × B heating becomes dominant in these operating conditions which is supposed to be insensitive to the electron density gradient scale length L/λ. Finally, an additional experimental study performed by changing the angle of incidence of the laser beam onto the solid target highlights a clear signature of the interplay between collisionless absorption mechanisms depending on the contrast ratio and intensity. Nature Publishing Group UK 2018-03-07 /pmc/articles/PMC5841281/ /pubmed/29515179 http://dx.doi.org/10.1038/s41598-018-22487-3 Text en © The Author(s) 2018 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 Azamoum, Y. Tcheremiskine, V. Clady, R. Ferré, A. Charmasson, L. Utéza, O. Sentis, M. Impact of the pulse contrast ratio on molybdenum K(α) generation by ultrahigh intensity femtosecond laser solid interaction |
title | Impact of the pulse contrast ratio on molybdenum K(α) generation by ultrahigh intensity femtosecond laser solid interaction |
title_full | Impact of the pulse contrast ratio on molybdenum K(α) generation by ultrahigh intensity femtosecond laser solid interaction |
title_fullStr | Impact of the pulse contrast ratio on molybdenum K(α) generation by ultrahigh intensity femtosecond laser solid interaction |
title_full_unstemmed | Impact of the pulse contrast ratio on molybdenum K(α) generation by ultrahigh intensity femtosecond laser solid interaction |
title_short | Impact of the pulse contrast ratio on molybdenum K(α) generation by ultrahigh intensity femtosecond laser solid interaction |
title_sort | impact of the pulse contrast ratio on molybdenum k(α) generation by ultrahigh intensity femtosecond laser solid interaction |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5841281/ https://www.ncbi.nlm.nih.gov/pubmed/29515179 http://dx.doi.org/10.1038/s41598-018-22487-3 |
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