Sebastián E. Nuza, Matthias Hoeft, Ana Contreras-Santos, Alexander Knebe, Gustavo Yepes
{"title":"The Three Hundred project: Radio luminosity evolution from merger-induced shock fronts in simulated galaxy clusters","authors":"Sebastián E. Nuza, Matthias Hoeft, Ana Contreras-Santos, Alexander Knebe, Gustavo Yepes","doi":"arxiv-2409.09422","DOIUrl":null,"url":null,"abstract":"Galaxy cluster mergers are believed to generate large-scale shock waves that\nare ideal sites for electron acceleration. We compute radio emission light\ncurves for galaxy group and cluster mergers simulated in a cosmological context\nto study the dependence of radio luminosity on cluster mass, redshift, and\nimpact parameter. We used model galaxy clusters from The Three Hundred project\nto identify cluster mergers characterised by the two main merging structures\nand follow their evolution throughout the simulated cosmic history. We found\nthat the median non-thermal radio relic luminosity light curve produced in\ngalaxy cluster mergers can be described by a skewed Gaussian function abruptly\nrising after core-passage of the secondary cluster that peaks after\n$\\sim0.1-0.8\\,$Gyr as a function of $M_{200,1}$, the mass of the primary,\ndisplaying a mass-dependent luminosity output increase of $\\lesssim10$ to about\n$\\gtrsim10-50$ times relative to the radio emission measured at core-passage\nfor galaxy groups and clusters, respectively. In general, most merger orbits\nare fairly radial with a median opening angle of $\\sim20^{\\circ}$ before the\ncollision. We also found that, independent of the cluster mass, less radial\nmergers tend to last longer, although the trend is weak. Finally, we found that\nthe peak radio luminosity shows a significant correlation with mass,\n$P_{1.4}\\propto M_{200,1}^{2.05}$, demonstrating that this relation holds all\nthe way up from galaxy group scales to the most massive galaxy clusters. We\nconclude that cluster mass is the primary driver for radio `gischt' median\nluminosity, although there are significant variations for a given cluster mass.\nOur simulations suggest that the shock-driven, non-thermal radio emission\nobserved on cluster outskirts are the result of massive galaxy cluster mergers\nat $z\\lesssim1$, peaking at $z\\sim0-0.5$.","PeriodicalId":501207,"journal":{"name":"arXiv - PHYS - Cosmology and Nongalactic Astrophysics","volume":"102 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Cosmology and Nongalactic Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.09422","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
Galaxy cluster mergers are believed to generate large-scale shock waves that
are ideal sites for electron acceleration. We compute radio emission light
curves for galaxy group and cluster mergers simulated in a cosmological context
to study the dependence of radio luminosity on cluster mass, redshift, and
impact parameter. We used model galaxy clusters from The Three Hundred project
to identify cluster mergers characterised by the two main merging structures
and follow their evolution throughout the simulated cosmic history. We found
that the median non-thermal radio relic luminosity light curve produced in
galaxy cluster mergers can be described by a skewed Gaussian function abruptly
rising after core-passage of the secondary cluster that peaks after
$\sim0.1-0.8\,$Gyr as a function of $M_{200,1}$, the mass of the primary,
displaying a mass-dependent luminosity output increase of $\lesssim10$ to about
$\gtrsim10-50$ times relative to the radio emission measured at core-passage
for galaxy groups and clusters, respectively. In general, most merger orbits
are fairly radial with a median opening angle of $\sim20^{\circ}$ before the
collision. We also found that, independent of the cluster mass, less radial
mergers tend to last longer, although the trend is weak. Finally, we found that
the peak radio luminosity shows a significant correlation with mass,
$P_{1.4}\propto M_{200,1}^{2.05}$, demonstrating that this relation holds all
the way up from galaxy group scales to the most massive galaxy clusters. We
conclude that cluster mass is the primary driver for radio `gischt' median
luminosity, although there are significant variations for a given cluster mass.
Our simulations suggest that the shock-driven, non-thermal radio emission
observed on cluster outskirts are the result of massive galaxy cluster mergers
at $z\lesssim1$, peaking at $z\sim0-0.5$.