Uphill acceleration in a spatially modulated electrostatic field particle accelerator
Autor(a) principal: | |
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Data de Publicação: | 2018 |
Outros Autores: | , , , , , |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UFRGS |
Texto Completo: | http://hdl.handle.net/10183/204117 |
Resumo: | Spatially modulated electrostatic fields can be designed to efficiently accelerate particles by exploring the relationships between the amplitude, the phase velocity, the shape of the potential, and the initial velocity of the particle. The acceleration process occurs when the value of the velocity excursions of the particle surpasses the phase velocity of the carrier, as a resonant mechanism. The ponderomotive approximation based on the Lagrangian average is usually applied in this kind of system in non-accelerating regimes. The mean dynamics of the particle is well described by this approximation far from resonance. However, the approximation fails to predict some interesting features of the model near resonance, such as the uphill acceleration phenomenon. A canonical perturbation theory is more accurate in these conditions. In this work, we compare the results from the Lagrangian average and from a canonical perturbation theory, focusing in regions where the results of these two approaches differ from each other. |
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Almansa, Ivanessa da SilveiraBurton, David A.Cairns, R.A.Marini, SamuelPeter, Eduardo AlcidesRizzato, Felipe BarbedoRussman, Felipe Boff2020-01-14T04:15:28Z20181070-664Xhttp://hdl.handle.net/10183/204117001109683Spatially modulated electrostatic fields can be designed to efficiently accelerate particles by exploring the relationships between the amplitude, the phase velocity, the shape of the potential, and the initial velocity of the particle. The acceleration process occurs when the value of the velocity excursions of the particle surpasses the phase velocity of the carrier, as a resonant mechanism. The ponderomotive approximation based on the Lagrangian average is usually applied in this kind of system in non-accelerating regimes. The mean dynamics of the particle is well described by this approximation far from resonance. However, the approximation fails to predict some interesting features of the model near resonance, such as the uphill acceleration phenomenon. A canonical perturbation theory is more accurate in these conditions. In this work, we compare the results from the Lagrangian average and from a canonical perturbation theory, focusing in regions where the results of these two approaches differ from each other.application/pdfengPhysics of plasmas. Melville. Vol. 25, no. 11 (Nov. 2018), 113107, 6 p.Aceleradores de partículasSimulação numéricaOndas eletrostáticasUphill acceleration in a spatially modulated electrostatic field particle acceleratorEstrangeiroinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFRGSinstname:Universidade Federal do Rio Grande do Sul (UFRGS)instacron:UFRGSTEXT001109683.pdf.txt001109683.pdf.txtExtracted Texttext/plain28274http://www.lume.ufrgs.br/bitstream/10183/204117/2/001109683.pdf.txtca1de2abd86709e3f5e9332dbe0e33d2MD52ORIGINAL001109683.pdfTexto completo (inglês)application/pdf1110892http://www.lume.ufrgs.br/bitstream/10183/204117/1/001109683.pdf8ebafd617537ef2f5a3f446b3bb93b5bMD5110183/2041172023-08-25 03:32:08.219937oai:www.lume.ufrgs.br:10183/204117Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2023-08-25T06:32:08Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false |
dc.title.pt_BR.fl_str_mv |
Uphill acceleration in a spatially modulated electrostatic field particle accelerator |
title |
Uphill acceleration in a spatially modulated electrostatic field particle accelerator |
spellingShingle |
Uphill acceleration in a spatially modulated electrostatic field particle accelerator Almansa, Ivanessa da Silveira Aceleradores de partículas Simulação numérica Ondas eletrostáticas |
title_short |
Uphill acceleration in a spatially modulated electrostatic field particle accelerator |
title_full |
Uphill acceleration in a spatially modulated electrostatic field particle accelerator |
title_fullStr |
Uphill acceleration in a spatially modulated electrostatic field particle accelerator |
title_full_unstemmed |
Uphill acceleration in a spatially modulated electrostatic field particle accelerator |
title_sort |
Uphill acceleration in a spatially modulated electrostatic field particle accelerator |
author |
Almansa, Ivanessa da Silveira |
author_facet |
Almansa, Ivanessa da Silveira Burton, David A. Cairns, R.A. Marini, Samuel Peter, Eduardo Alcides Rizzato, Felipe Barbedo Russman, Felipe Boff |
author_role |
author |
author2 |
Burton, David A. Cairns, R.A. Marini, Samuel Peter, Eduardo Alcides Rizzato, Felipe Barbedo Russman, Felipe Boff |
author2_role |
author author author author author author |
dc.contributor.author.fl_str_mv |
Almansa, Ivanessa da Silveira Burton, David A. Cairns, R.A. Marini, Samuel Peter, Eduardo Alcides Rizzato, Felipe Barbedo Russman, Felipe Boff |
dc.subject.por.fl_str_mv |
Aceleradores de partículas Simulação numérica Ondas eletrostáticas |
topic |
Aceleradores de partículas Simulação numérica Ondas eletrostáticas |
description |
Spatially modulated electrostatic fields can be designed to efficiently accelerate particles by exploring the relationships between the amplitude, the phase velocity, the shape of the potential, and the initial velocity of the particle. The acceleration process occurs when the value of the velocity excursions of the particle surpasses the phase velocity of the carrier, as a resonant mechanism. The ponderomotive approximation based on the Lagrangian average is usually applied in this kind of system in non-accelerating regimes. The mean dynamics of the particle is well described by this approximation far from resonance. However, the approximation fails to predict some interesting features of the model near resonance, such as the uphill acceleration phenomenon. A canonical perturbation theory is more accurate in these conditions. In this work, we compare the results from the Lagrangian average and from a canonical perturbation theory, focusing in regions where the results of these two approaches differ from each other. |
publishDate |
2018 |
dc.date.issued.fl_str_mv |
2018 |
dc.date.accessioned.fl_str_mv |
2020-01-14T04:15:28Z |
dc.type.driver.fl_str_mv |
Estrangeiro info:eu-repo/semantics/article |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://hdl.handle.net/10183/204117 |
dc.identifier.issn.pt_BR.fl_str_mv |
1070-664X |
dc.identifier.nrb.pt_BR.fl_str_mv |
001109683 |
identifier_str_mv |
1070-664X 001109683 |
url |
http://hdl.handle.net/10183/204117 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.ispartof.pt_BR.fl_str_mv |
Physics of plasmas. Melville. Vol. 25, no. 11 (Nov. 2018), 113107, 6 p. |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
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application/pdf |
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