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A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator
Laser wakefield accelerators (LWFAs) can produce high-energy electron bunches in short distances. Successfully coupling these sources with undulators has the potential to form an LWFA-driven free-electron laser (FEL), providing high-intensity short-wavelength radiation. Electron bunches produced fro...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10232591/ https://www.ncbi.nlm.nih.gov/pubmed/37258601 http://dx.doi.org/10.1038/s41598-023-35435-7 |
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author | Dewhurst, Kay A. Muratori, Bruno D. Brunetti, Enrico van der Geer, Bas de Loos, Marieke Owen, Hywel L. Wiggins, S. Mark Jaroszynski, Dino A. |
author_facet | Dewhurst, Kay A. Muratori, Bruno D. Brunetti, Enrico van der Geer, Bas de Loos, Marieke Owen, Hywel L. Wiggins, S. Mark Jaroszynski, Dino A. |
author_sort | Dewhurst, Kay A. |
collection | PubMed |
description | Laser wakefield accelerators (LWFAs) can produce high-energy electron bunches in short distances. Successfully coupling these sources with undulators has the potential to form an LWFA-driven free-electron laser (FEL), providing high-intensity short-wavelength radiation. Electron bunches produced from LWFAs have a correlated distribution in longitudinal phase space: a chirp. However, both LWFAs and FELs have strict parameter requirements. The bunch chirp created using ideal LWFA parameters may not suit the FEL; for example, a chirp can reduce the high peak current required for free-electron lasing. We, therefore, design a flexible beamline that can accept either positively or negatively chirped LWFA bunches and adjust the chirp during transport to an undulator. We have used the accelerator design program MAD8 to design a beamline in stages, and to track particle bunches. The final beamline design can produce ambidirectional values of longitudinal dispersion ([Formula: see text] ): we demonstrate values of + 0.20 mm, 0.00 mm and − 0.22 mm. Positive or negative values of [Formula: see text] apply a shear forward or backward in the longitudinal phase space of the electron bunch, which provides control of the bunch chirp. This chirp control during the bunch transport gives an additional free parameter and marks a new approach to matching future LWFA-driven FELs. |
format | Online Article Text |
id | pubmed-10232591 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-102325912023-06-02 A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator Dewhurst, Kay A. Muratori, Bruno D. Brunetti, Enrico van der Geer, Bas de Loos, Marieke Owen, Hywel L. Wiggins, S. Mark Jaroszynski, Dino A. Sci Rep Article Laser wakefield accelerators (LWFAs) can produce high-energy electron bunches in short distances. Successfully coupling these sources with undulators has the potential to form an LWFA-driven free-electron laser (FEL), providing high-intensity short-wavelength radiation. Electron bunches produced from LWFAs have a correlated distribution in longitudinal phase space: a chirp. However, both LWFAs and FELs have strict parameter requirements. The bunch chirp created using ideal LWFA parameters may not suit the FEL; for example, a chirp can reduce the high peak current required for free-electron lasing. We, therefore, design a flexible beamline that can accept either positively or negatively chirped LWFA bunches and adjust the chirp during transport to an undulator. We have used the accelerator design program MAD8 to design a beamline in stages, and to track particle bunches. The final beamline design can produce ambidirectional values of longitudinal dispersion ([Formula: see text] ): we demonstrate values of + 0.20 mm, 0.00 mm and − 0.22 mm. Positive or negative values of [Formula: see text] apply a shear forward or backward in the longitudinal phase space of the electron bunch, which provides control of the bunch chirp. This chirp control during the bunch transport gives an additional free parameter and marks a new approach to matching future LWFA-driven FELs. Nature Publishing Group UK 2023-05-31 /pmc/articles/PMC10232591/ /pubmed/37258601 http://dx.doi.org/10.1038/s41598-023-35435-7 Text en © The Author(s) 2023 https://creativecommons.org/licenses/by/4.0/Open AccessThis 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 licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence 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 licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Article Dewhurst, Kay A. Muratori, Bruno D. Brunetti, Enrico van der Geer, Bas de Loos, Marieke Owen, Hywel L. Wiggins, S. Mark Jaroszynski, Dino A. A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator |
title | A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator |
title_full | A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator |
title_fullStr | A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator |
title_full_unstemmed | A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator |
title_short | A beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator |
title_sort | beamline to control longitudinal phase space whilst transporting laser wakefield accelerated electrons to an undulator |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10232591/ https://www.ncbi.nlm.nih.gov/pubmed/37258601 http://dx.doi.org/10.1038/s41598-023-35435-7 |
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