The emergence of the first star-free atomic cooling haloes in the Universe

Author:

Regan John A1ORCID,Wise John H2,O’Shea Brian W3456,Norman Michael L7

Affiliation:

1. Centre for Astrophysics and Relativity, School of Mathematical Sciences, Dublin City University, Glasnevin D09 W6Y4, Ireland

2. Center for Relativistic Astrophysics, Georgia Institute of Technology, 837 State Street, Atlanta, GA 30332, USA

3. National Superconducting Cyclotron Laboratory, Michigan State University, 640 S Shaw Ln, East Lansing, MI 48823, USA

4. Department of Physics and Astronomy, Michigan State University, 567 Wilson Rd, East Lansing, MI 48823, USA

5. Department of Computational Mathematics, Science and Engineering, Michigan State University, 428 S Shaw Ln, East Lansing, MI 48823, USA

6. Joint Institute for Nuclear Astrophysics - Center for the Evolution of the Elements, 640 S Shaw Lane, East Lansing, MI 48824, USA

7. Center for Astrophysics and Space Sciences, University of California, San Diego, 9500 Gilman Dr, La Jolla, CA 92093, USA

Abstract

ABSTRACT Using the Renaissance suite of simulations, we examine the emergence of pristine atomic cooling haloes that are both metal free and star free in the early universe. The absence of metals prevents catastrophic cooling, suppresses fragmentation, and may allow for the formation of massive black hole seeds. Here we report on the abundance of pristine atomic cooling haloes found and on the specific physical conditions that allow for the formation of these direct-collapse-black hole (DCBH) haloes. In total, in our simulations we find that 79 DCBH haloes form before a redshift of 11.6. We find that the formation of pristine atomic haloes is driven by the rapid assembly of the atomic cooling haloes with mergers, both minor and/or major, prior to reaching the atomic cooling limit a requirement. However, the ability of assembling haloes to remain free of (external) metal enrichment is equally important and underlines the necessity of following the transport of metals in such simulations. The candidate DCBH-hosting haloes we find have been exposed to mean Lyman–Werner radiation fields of J21 ∼1 and typically lie at least 10 kpc (physical) from the nearest massive galaxy. The growth rates of the haloes reach values of greater than 107$\rm {M_{\odot }}~$ per unit redshift, leading to significant dynamical heating and the suppression of efficient cooling until the halo crosses the atomic cooling threshold. Finally, we also find five synchronized halo candidates where pairs of pristine atomic cooling haloes emerge that are both spatially and temporally synchronized.

Funder

NSF

NASA

National Centre for Supercomputing Applications

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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