Galaxy formation with BECDM – II. Cosmic filaments and first galaxies

Author:

Mocz Philip1ORCID,Fialkov Anastasia2,Vogelsberger Mark3ORCID,Becerra Fernando4ORCID,Shen Xuejian5,Robles Victor H6ORCID,Amin Mustafa A7,Zavala Jesús8,Boylan-Kolchin Michael9ORCID,Bose Sownak4ORCID,Marinacci Federico10ORCID,Chavanis Pierre-Henri11,Lancaster Lachlan1ORCID,Hernquist Lars4

Affiliation:

1. Department of Astrophysical Sciences, Princeton University, 4 Ivy Lane, Princeton, NJ 08544, USA

2. Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA, UK

3. Department of Physics, Kavli Institute for Astrophysics and Space Research, M.I.T., Cambridge, MA 02139, USA

4. Harvard–Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USA

5. TAPIR, California Institute of Technology, Pasadena, CA 91125, USA

6. Department of Physics and Astronomy, University of California, Irvine, CA 92697, USA

7. Physics & Astronomy Department, Rice University, Houston, TX 77005-1827, USA

8. Center for Astrophysics and Cosmology, Science Institute, University of Iceland, Dunhagi 5, 107 Reykjavik, Iceland

9. Department of Astronomy, The University of Texas at Austin, 2515 Speedway, Stop C1400, Austin, TX 78712-1205, USA

10. Department of Physics & Astronomy, University of Bologna, via Gobetti 93/2, I-40129 Bologna, Italy

11. Laboratoire de Physique Théorique, CNRS, Université Paul Sabatier, 118 route de Narbonne, F-31062 Toulouse, France

Abstract

ABSTRACT Bose–Einstein condensate dark matter (BECDM, also known as fuzzy dark matter) 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 × 10−22 eV, exploring the dynamical effects of its wavelike nature on the cosmic web and the formation of first galaxies. Our BECDM simulations are directly compared to CDM as well 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.

Funder

National Aeronautics and Space Administration

National Sleep Foundation

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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