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Laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection
In the few-cycle pulse regime of laser-cluster interaction (intensity [Formula: see text] , wavelength [Formula: see text] nm), laser absorption is mostly collisionless and may happen via anharmonic resonance (AHR) process in the overdense (cluster) plasma potential. Many experiments, theory and si...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9253368/ https://www.ncbi.nlm.nih.gov/pubmed/35787644 http://dx.doi.org/10.1038/s41598-022-14816-4 |
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author | Swain, Kalyani Mahalik, Sagar Sekhar Kundu, Mrityunjay |
author_facet | Swain, Kalyani Mahalik, Sagar Sekhar Kundu, Mrityunjay |
author_sort | Swain, Kalyani |
collection | PubMed |
description | In the few-cycle pulse regime of laser-cluster interaction (intensity [Formula: see text] , wavelength [Formula: see text] nm), laser absorption is mostly collisionless and may happen via anharmonic resonance (AHR) process in the overdense (cluster) plasma potential. Many experiments, theory and simulation show average absorbed energy per cluster-electron ([Formula: see text] ) close to the electron’s ponderomotive energy ([Formula: see text] ) in the collisionless regime. In this work, by simple rigid sphere model (RSM) and detailed particle-in-cell (PIC) simulation, we show enhanced [Formula: see text] 30–70[Formula: see text] —a 15–30 fold increase—with an external (crossed) magnetic field near the electron-cyclotron resonance (ECR). Due to relativistic mass increase, electrons quickly deviate from the standard (non-relativistic) ECR, but time-dependent relativistic-ECR (RECR) happens which also contributes to enhanced [Formula: see text] . Here laser is coupled to electrons in two stages, i.e, AHR and ECR/RECR. To probe further we retrieve the phase-difference [Formula: see text] between the driving electric field and corresponding velocity component for each electron (in PIC and RSM). We find absorption by electron via AHR happens in a very short interval [Formula: see text] for less than half a laser period where [Formula: see text] remains close to [Formula: see text] (necessary condition for maximum laser absorption) and then [Formula: see text] drops to its initial [Formula: see text] (meaning no absorption) after such short-lived AHR. On the contrary, auxiliary magnetic field near the ECR modifies AHR scenario inside the cluster and also helps maintaining the required phase [Formula: see text] for the liberated cluster-electron accompanied by frequency matching for ECR/RECR for a prolonged [Formula: see text] (which covers 50–60% of the laser pulse through pulse maxima) even after AHR—leading to jump in [Formula: see text] 30–70[Formula: see text] . We note that to realize the second stage of enhanced energy coupling via ECR/RECR, the first stage via AHR is necessary. |
format | Online Article Text |
id | pubmed-9253368 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-92533682022-07-06 Laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection Swain, Kalyani Mahalik, Sagar Sekhar Kundu, Mrityunjay Sci Rep Article In the few-cycle pulse regime of laser-cluster interaction (intensity [Formula: see text] , wavelength [Formula: see text] nm), laser absorption is mostly collisionless and may happen via anharmonic resonance (AHR) process in the overdense (cluster) plasma potential. Many experiments, theory and simulation show average absorbed energy per cluster-electron ([Formula: see text] ) close to the electron’s ponderomotive energy ([Formula: see text] ) in the collisionless regime. In this work, by simple rigid sphere model (RSM) and detailed particle-in-cell (PIC) simulation, we show enhanced [Formula: see text] 30–70[Formula: see text] —a 15–30 fold increase—with an external (crossed) magnetic field near the electron-cyclotron resonance (ECR). Due to relativistic mass increase, electrons quickly deviate from the standard (non-relativistic) ECR, but time-dependent relativistic-ECR (RECR) happens which also contributes to enhanced [Formula: see text] . Here laser is coupled to electrons in two stages, i.e, AHR and ECR/RECR. To probe further we retrieve the phase-difference [Formula: see text] between the driving electric field and corresponding velocity component for each electron (in PIC and RSM). We find absorption by electron via AHR happens in a very short interval [Formula: see text] for less than half a laser period where [Formula: see text] remains close to [Formula: see text] (necessary condition for maximum laser absorption) and then [Formula: see text] drops to its initial [Formula: see text] (meaning no absorption) after such short-lived AHR. On the contrary, auxiliary magnetic field near the ECR modifies AHR scenario inside the cluster and also helps maintaining the required phase [Formula: see text] for the liberated cluster-electron accompanied by frequency matching for ECR/RECR for a prolonged [Formula: see text] (which covers 50–60% of the laser pulse through pulse maxima) even after AHR—leading to jump in [Formula: see text] 30–70[Formula: see text] . We note that to realize the second stage of enhanced energy coupling via ECR/RECR, the first stage via AHR is necessary. Nature Publishing Group UK 2022-07-04 /pmc/articles/PMC9253368/ /pubmed/35787644 http://dx.doi.org/10.1038/s41598-022-14816-4 Text en © The Author(s) 2022 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 Swain, Kalyani Mahalik, Sagar Sekhar Kundu, Mrityunjay Laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection |
title | Laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection |
title_full | Laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection |
title_fullStr | Laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection |
title_full_unstemmed | Laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection |
title_short | Laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection |
title_sort | laser cluster interaction in ambient magnetic fields for accelerating electrons in two stages without external injection |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9253368/ https://www.ncbi.nlm.nih.gov/pubmed/35787644 http://dx.doi.org/10.1038/s41598-022-14816-4 |
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