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dc.contributor.authorMocz, Philip
dc.contributor.authorFialkov, Anastasia
dc.contributor.authorVogelsberger, Mark
dc.contributor.authorBecerra, Fernando
dc.contributor.authorShen, Xuejian
dc.contributor.authorRobles, Victor H
dc.contributor.authorAmin, Mustafa A
dc.contributor.authorZavala, Jesús
dc.contributor.authorBoylan-Kolchin, Michael
dc.contributor.authorBose, Sownak
dc.contributor.authorMarinacci, Federico
dc.contributor.authorChavanis, Pierre-Henri
dc.contributor.authorLancaster, Lachlan
dc.contributor.authorHernquist, Lars
dc.date.accessioned2021-09-20T18:23:04Z
dc.date.available2021-09-20T18:23:04Z
dc.date.issued2020
dc.identifier.urihttps://hdl.handle.net/1721.1/132565
dc.description.abstract© 2020 Oxford University Press. All rights reserved. Bose-Einstein condensate darkmatter (BECDM,also known as fuzzy darkmatter) is motivated by fundamental physics and has recently received significant attention as a serious alternative to the established cold dark matter (CDM) model. We perform cosmological simulations of BECDM gravitationally coupled to baryons and investigate structure formation at high redshifts (z ≥ 5) for a boson mass m = 2.5 ×10-22eV, exploring the dynamical effects of its wavelike nature on the cosmicweb and the formation of first galaxies.OurBECDMsimulations are directly compared toCDMaswell as to simulations where the dynamical quantum potential is ignored and only the initial suppression of the power spectrum is considered - a warm dark matter-like ('WDM') model often used as a proxy for BECDM. Our simulations confirm that 'WDM' is a good approximation to BECDM on large cosmological scales even in the presence of the baryonic feedback. Similarities also exist on small scales, with primordial star formation happening both in isolated haloes and continuously along cosmic filaments; the latter effect is not present in CDM. Global star formation and metal enrichment in these first galaxies are delayed in BECDM/'WDM' compared to the CDM case: in BECDM/'WDM' first stars form at z ~ 13/13.5, while in CDM star formation starts at z ~ 35. The signature of BECDM interference, not present in 'WDM', is seen in the evolved dark matter power spectrum: although the small-scale structure is initially suppressed, power on kpc scales is added at lower redshifts. Our simulations lay the groundwork for realistic simulations of galaxy formation in BECDM.
dc.language.isoen
dc.publisherOxford University Press (OUP)
dc.relation.isversionof10.1093/MNRAS/STAA738
dc.rightsCreative Commons Attribution-Noncommercial-Share Alike
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/4.0/
dc.sourcearXiv
dc.titleGalaxy formation with BECDM – II. Cosmic filaments and first galaxies
dc.typeArticle
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.contributor.departmentMIT Kavli Institute for Astrophysics and Space Research
dc.relation.journalMonthly Notices of the Royal Astronomical Society
dc.eprint.versionOriginal manuscript
dc.type.urihttp://purl.org/eprint/type/JournalArticle
eprint.statushttp://purl.org/eprint/status/NonPeerReviewed
dc.date.updated2020-11-17T15:35:11Z
dspace.orderedauthorsMocz, P; Fialkov, A; Vogelsberger, M; Becerra, F; Shen, X; Robles, VH; Amin, MA; Zavala, J; Boylan-Kolchin, M; Bose, S; Marinacci, F; Chavanis, P-H; Lancaster, L; Hernquist, L
dspace.date.submission2020-11-17T15:35:20Z
mit.journal.volume494
mit.journal.issue2
mit.licenseOPEN_ACCESS_POLICY
mit.metadata.statusAuthority Work and Publication Information Needed


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