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dc.contributor.authorMartizzi, Davide
dc.contributor.authorVogelsberger, Mark
dc.contributor.authorArtale, Maria Celeste
dc.contributor.authorHaider, Markus
dc.contributor.authorTorrey, Paul A.
dc.contributor.authorMarinacci, Federico
dc.contributor.authorNelson, Dylan
dc.contributor.authorPillepich, Annalisa
dc.contributor.authorWeinberger, Rainer
dc.contributor.authorHernquist, Lars
dc.contributor.authorNaiman, Jill
dc.contributor.authorSpringel, Volker
dc.date.accessioned2022-08-03T18:02:44Z
dc.date.available2021-09-20T18:23:12Z
dc.date.available2022-08-03T18:02:44Z
dc.date.issued2019
dc.identifier.urihttps://hdl.handle.net/1721.1/132588.2
dc.description.abstract© 2019 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society. We analyse the IllustrisTNG simulations to study the mass, volume fraction, and phase distribution of gaseous baryons embedded in the knots, filaments, sheets, and voids of the Cosmic Web from redshift z = 8 to redshift z = 0. We find that filaments host more star-forming gas than knots, and that filaments also have a higher relative mass fraction of gas in this phase than knots. We also show that the cool, diffuse intergalactic medium [IGM; $T\lt 105 \, {\rm K}$, $n-{\rm H}\lt 10{-4}(1+z) \, {\rm cm{-3}}$] and the warm-hot intergalactic medium [WHIM; $105 \lt T\lt 107 \, {\rm K}$, $n-{\rm H} \lt 10{-4}(1+z)\, {\rm cm{-3}}$] constitute ${\sim } 39$ and ${\sim } 46{{\ \rm per\ cent}}$ of the baryons at redshift z = 0, respectively. Our results indicate that the WHIM may constitute the largest reservoir of missing baryons at redshift z = 0. Using our Cosmic Web classification, we predict the WHIM to be the dominant baryon mass contribution in filaments and knots at redshift z = 0, but not in sheets and voids where the cool, diffuse IGM dominates. We also characterize the evolution of WHIM and IGM from redshift z = 4 to redshift z = 0, and find that the mass fraction of WHIM in filaments and knots evolves only by a factor of ∼2 from redshift z = 0 to 1, but declines faster at higher redshift. The WHIM only occupies $4\!-\!11{{\ \rm per\ cent}}$ of the volume at redshift 0 ≤ z ≤ 1. We predict the existence of a significant number of currently undetected O vii and Ne ix absorption systems in cosmic filaments, which could be detected by future X-ray telescopes like Athena.en_US
dc.language.isoen
dc.publisherOxford University Press (OUP)en_US
dc.relation.isversionof10.1093/MNRAS/STZ1106en_US
dc.rightsCreative Commons Attribution-Noncommercial-Share Alikeen_US
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/4.0/en_US
dc.sourcearXiven_US
dc.titleBaryons in the Cosmic Web of IllustrisTNG – I: gas in knots, filaments, sheets, and voidsen_US
dc.typeArticleen_US
dc.contributor.departmentMIT Kavli Institute for Astrophysics and Space Researchen_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physicsen_US
dc.relation.journalMonthly Notices of the Royal Astronomical Societyen_US
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2020-11-12T18:13:21Z
dspace.orderedauthorsMartizzi, D; Vogelsberger, M; Artale, MC; Haider, M; Torrey, P; Marinacci, F; Nelson, D; Pillepich, A; Weinberger, R; Hernquist, L; Naiman, J; Springel, Ven_US
dspace.date.submission2020-11-12T18:13:37Z
mit.journal.volume486en_US
mit.journal.issue3en_US
mit.metadata.statusPublication Information Neededen_US


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