3D PIC Simulations for relativistic jets with a toroidal magnetic field
We have investigated how kinetic instabilities such as the Weibel instability (WI), the mushroom instability (MI), and the kinetic Kelvin–Helmholtz instability (kKHI) are excited in jets without and with a toroidal magnetic field, and how such instabilities contribute to particle acceleration. In th...
| Autores: | , , , , , , , , |
|---|---|
| Tipo de recurso: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2023 |
| País: | España |
| Institución: | Consejo Superior de Investigaciones Científicas (CSIC) |
| Repositorio: | DIGITAL.CSIC. Repositorio Institucional del CSIC |
| OAI Identifier: | oai:digital.csic.es:10261/307547 |
| Acceso en línea: | http://hdl.handle.net/10261/307547 |
| Access Level: | acceso abierto |
| Palabra clave: | Acceleration of particles Instabilities Relativistic processes Shock waves Galaxies: jets |
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| dc.title.none.fl_str_mv |
3D PIC Simulations for relativistic jets with a toroidal magnetic field |
| title |
3D PIC Simulations for relativistic jets with a toroidal magnetic field |
| spellingShingle |
3D PIC Simulations for relativistic jets with a toroidal magnetic field Meli, Athina Acceleration of particles Instabilities Relativistic processes Shock waves Galaxies: jets |
| title_short |
3D PIC Simulations for relativistic jets with a toroidal magnetic field |
| title_full |
3D PIC Simulations for relativistic jets with a toroidal magnetic field |
| title_fullStr |
3D PIC Simulations for relativistic jets with a toroidal magnetic field |
| title_full_unstemmed |
3D PIC Simulations for relativistic jets with a toroidal magnetic field |
| title_sort |
3D PIC Simulations for relativistic jets with a toroidal magnetic field |
| dc.creator.none.fl_str_mv |
Meli, Athina Nishikawa, Kenichi Köhn, Christoph Duţan, Ioana Mizuno, Yosuke Kobzar, Oleh MacDonald, Nicholas Gómez Fernández, José L. Hirotani, Kouichi |
| author |
Meli, Athina |
| author_facet |
Meli, Athina Nishikawa, Kenichi Köhn, Christoph Duţan, Ioana Mizuno, Yosuke Kobzar, Oleh MacDonald, Nicholas Gómez Fernández, José L. Hirotani, Kouichi |
| author_role |
author |
| author2 |
Nishikawa, Kenichi Köhn, Christoph Duţan, Ioana Mizuno, Yosuke Kobzar, Oleh MacDonald, Nicholas Gómez Fernández, José L. Hirotani, Kouichi |
| author2_role |
author author author author author author author author |
| dc.contributor.none.fl_str_mv |
Ministerio de Ciencia e Innovación (España) Junta de Andalucía European Commission NASA Consejo Superior de Investigaciones Científicas [https://ror.org/02gfc7t72] |
| dc.subject.none.fl_str_mv |
Acceleration of particles Instabilities Relativistic processes Shock waves Galaxies: jets |
| topic |
Acceleration of particles Instabilities Relativistic processes Shock waves Galaxies: jets |
| description |
We have investigated how kinetic instabilities such as the Weibel instability (WI), the mushroom instability (MI), and the kinetic Kelvin–Helmholtz instability (kKHI) are excited in jets without and with a toroidal magnetic field, and how such instabilities contribute to particle acceleration. In this work, we use a new jet injection scheme, where an electric current is self-consistently generated at the jet orifice by the jet particles, which produce the toroidal magnetic field. We perform five different simulations for a sufficiently long time to examine the non-linear effects of the jet evolution. We inject unmagnetized e± and e−– p+ (mp/me = 1836), as well as magnetized e± and e−– i+ (mi/me = 4) jets with a top-hat jet density profile into an unmagnetized ambient plasmas of the same species. We show that WI, MI, and kKHI excited at the linear stage, generate a non-oscillatory x-component of the electric field accelerating, and decelerating electrons. We find that the two different jet compositions (e± and e−– i+) display different instability modes, respectively. Moreover, the magnetic field in the non-linear stage generated by different instabilities is dissipated and reorganized into new topologies. A 3D magnetic field topology depiction indicates possible reconnection sites in the non-linear stage, where the particles are significantly accelerated by the dissipation of the magnetic field associated to a possible reconnection event. © 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society. |
| publishDate |
2023 |
| dc.date.none.fl_str_mv |
2023 2023 2023 |
| dc.type.none.fl_str_mv |
info:eu-repo/semantics/article http://purl.org/coar/resource_type/c_6501 Publisher's version info:eu-repo/semantics/publishedVersion |
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article |
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publishedVersion |
| dc.identifier.none.fl_str_mv |
http://hdl.handle.net/10261/307547 |
| url |
http://hdl.handle.net/10261/307547 |
| dc.language.none.fl_str_mv |
Inglés |
| language_invalid_str_mv |
Inglés |
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info:eu-repo/semantics/openAccess |
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openAccess |
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Oxford University Press |
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Oxford University Press |
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reponame:DIGITAL.CSIC. Repositorio Institucional del CSIC instname:Consejo Superior de Investigaciones Científicas (CSIC) |
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Consejo Superior de Investigaciones Científicas (CSIC) |
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DIGITAL.CSIC. Repositorio Institucional del CSIC |
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DIGITAL.CSIC. Repositorio Institucional del CSIC |
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1869420232270938112 |
| spelling |
3D PIC Simulations for relativistic jets with a toroidal magnetic fieldMeli, AthinaNishikawa, KenichiKöhn, ChristophDuţan, IoanaMizuno, YosukeKobzar, OlehMacDonald, NicholasGómez Fernández, José L.Hirotani, KouichiAcceleration of particlesInstabilitiesRelativistic processesShock wavesGalaxies: jetsWe have investigated how kinetic instabilities such as the Weibel instability (WI), the mushroom instability (MI), and the kinetic Kelvin–Helmholtz instability (kKHI) are excited in jets without and with a toroidal magnetic field, and how such instabilities contribute to particle acceleration. In this work, we use a new jet injection scheme, where an electric current is self-consistently generated at the jet orifice by the jet particles, which produce the toroidal magnetic field. We perform five different simulations for a sufficiently long time to examine the non-linear effects of the jet evolution. We inject unmagnetized e± and e−– p+ (mp/me = 1836), as well as magnetized e± and e−– i+ (mi/me = 4) jets with a top-hat jet density profile into an unmagnetized ambient plasmas of the same species. We show that WI, MI, and kKHI excited at the linear stage, generate a non-oscillatory x-component of the electric field accelerating, and decelerating electrons. We find that the two different jet compositions (e± and e−– i+) display different instability modes, respectively. Moreover, the magnetic field in the non-linear stage generated by different instabilities is dissipated and reorganized into new topologies. A 3D magnetic field topology depiction indicates possible reconnection sites in the non-linear stage, where the particles are significantly accelerated by the dissipation of the magnetic field associated to a possible reconnection event. © 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society.This work was supported by the National Aeronautics and Space Administration (NASA)-NNX12AH06G, NNX13AP-21G, and NNX13AP14G grants. Recent work was also provided by the NASA through Chandra Award Number GO7-18118X (PI: Ming Sun at UAH) issued by the Chandra X-ray Center, which is operated by the SAO for and on behalf of the NASA under contract NAS8-03060. The simulations presented in this report have been performed by Frontera supercomputer at the Texas Advanced Computing Center under the AST21038: Computational Study of Astrophysical Plasmas, and also provided by the NASA through by the grant: Nature Of Hard X-rays From A TeV-detected RadioGalaxy (PI: Ka Wah Wong at SUNY Brockport) issued by the NuSTAR Guest Observer Cycle 6 2019. Y.M. is supported by the ERC Synergy Grant ‘BlackHoleCam: Imaging the Event Horizon of Black Holes’ (Grant No. 610058). The work of I.D. has been supported by the NUCLEU project. Simulations were performed using Pleiades and Endeavor facilities at NASA Advanced Supercomputing (NAS: s2004), using Comet at The San Diego Supercomputer Center (SDSC), and Bridges at the Pittsburgh Supercomputing Center, which are supported by the National Science Foundation (NSF). JLG acknowledges the support of the Spanish Ministerio de Economía y Competitividad (grants AYA2016-80889-P, PID2019-108995GB-C21), the Consejería de Economía, Conocimiento, Empresas y Universidad, Junta de Andalucía (grant P18-FR-1769), the Consejo Superior de Investigaciones Científicas (grant 2019AEP112), and the State Agency for Research of the Spanish MCIU through the Center of Excellence Severo Ochoa award for the Instituto de Astrofísica de Andalucía (SEV-2017-0709).With funding from the Spanish government through the "Severo Ochoa Centre of Excellence" accreditation (SEV-2017-0709).Peer reviewedOxford University PressMinisterio de Ciencia e Innovación (España)Junta de AndalucíaEuropean CommissionNASAConsejo Superior de Investigaciones Científicas [https://ror.org/02gfc7t72]202320232023info:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_6501Publisher's versioninfo:eu-repo/semantics/publishedVersionhttp://hdl.handle.net/10261/307547reponame:DIGITAL.CSIC. Repositorio Institucional del CSICinstname:Consejo Superior de Investigaciones Científicas (CSIC)Inglés#PLACEHOLDER_PARENT_METADATA_VALUE##PLACEHOLDER_PARENT_METADATA_VALUE##PLACEHOLDER_PARENT_METADATA_VALUE#info:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2013-2016/SEV-2017-0709info:eu-repo/grantAgreement/MINECO//AYA2016-80889-Pinfo:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2017-2020/PID2019-108995GB-C21http://hdl.handle.net/10261/359865http://dx.doi.org/10.1093/mnras/stac3474Síinfo:eu-repo/semantics/openAccessoai:digital.csic.es:10261/3075472026-05-22T06:33:51Z |
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15.81155 |