Joana A kramer, Nicholas R. MacDonals, Georgios F. Paraschos, L. Ricci
{"title":"3D hybrid fluid-particle jet simulations and the importance of synchrotron radiative losses","authors":"Joana A kramer, Nicholas R. MacDonals, Georgios F. Paraschos, L. Ricci","doi":"arxiv-2409.05256","DOIUrl":null,"url":null,"abstract":"Context. Relativistic jets in active galactic nuclei are known for their\nexceptional energy output, and imaging the synthetic synchrotron emission of\nnumerical jet simulations is essential for a comparison with observed jet\npolarization emission. Aims. Through the use of 3D hybrid fluid-particle jet\nsimulations (with the PLUTO code), we overcome some of the commonly made\nassumptions in relativistic magnetohydrodynamic (RMHD) simulations by using\nnon-thermal particle attributes to account for the resulting synchrotron\nradiation. Polarized radiative transfer and ray-tracing (via the RADMC-3D code)\nhighlight the differences in total intensity maps when (i) the jet is simulated\npurely with the RMHD approach, (ii) a jet tracer is considered in the RMHD\napproach, and (iii) a hybrid fluid-particle approach is used. The resulting\nemission maps were compared to the example of the radio galaxy Centaurus A.\nMethods. We applied the Lagrangian particle module implemented in the latest\nversion of the PLUTO code. This new module contains a state-of-the-art\nalgorithm for modeling diffusive shock acceleration and for accounting for\nradiative losses in RMHD jet simulations. The module implements the physical\npostulates missing in RMHD jet simulations by accounting for a cooled ambient\nmedium and strengthening the central jet emission. Results. We find a\ndistinction between the innermost structure of the jet and the back-flowing\nmaterial by mimicking the radio emission of the Seyfert II radio galaxy\nCentaurus A when considering an edge-brightened jet with an underlying purely\ntoroidal magnetic field. We demonstrate the necessity of synchrotron cooling as\nwell as the improvements gained when directly accounting for non-thermal\nsynchrotron radiation via non-thermal particles.","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"12 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Astrophysical Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.05256","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Context. Relativistic jets in active galactic nuclei are known for their
exceptional energy output, and imaging the synthetic synchrotron emission of
numerical jet simulations is essential for a comparison with observed jet
polarization emission. Aims. Through the use of 3D hybrid fluid-particle jet
simulations (with the PLUTO code), we overcome some of the commonly made
assumptions in relativistic magnetohydrodynamic (RMHD) simulations by using
non-thermal particle attributes to account for the resulting synchrotron
radiation. Polarized radiative transfer and ray-tracing (via the RADMC-3D code)
highlight the differences in total intensity maps when (i) the jet is simulated
purely with the RMHD approach, (ii) a jet tracer is considered in the RMHD
approach, and (iii) a hybrid fluid-particle approach is used. The resulting
emission maps were compared to the example of the radio galaxy Centaurus A.
Methods. We applied the Lagrangian particle module implemented in the latest
version of the PLUTO code. This new module contains a state-of-the-art
algorithm for modeling diffusive shock acceleration and for accounting for
radiative losses in RMHD jet simulations. The module implements the physical
postulates missing in RMHD jet simulations by accounting for a cooled ambient
medium and strengthening the central jet emission. Results. We find a
distinction between the innermost structure of the jet and the back-flowing
material by mimicking the radio emission of the Seyfert II radio galaxy
Centaurus A when considering an edge-brightened jet with an underlying purely
toroidal magnetic field. We demonstrate the necessity of synchrotron cooling as
well as the improvements gained when directly accounting for non-thermal
synchrotron radiation via non-thermal particles.