The influence of subhaloes on host halo properties

Author:

Mezini Lorena12ORCID,Fielder Catherine E3ORCID,Zentner Andrew R12ORCID,Mao Yao-Yuan4ORCID,Wang Kuan56ORCID,Wu Hao-Yi7

Affiliation:

1. Department of Physics and Astronomy, University of Pittsburgh , Pittsburgh, PA 15260, USA

2. Pittsburgh Particle Physics, Astrophysics, and Cosmology Center (PITT PACC), University of Pittsburgh , Pittsburgh, PA 15260, USA

3. Steward Observatory, University of Arizona , Tucson, AZ 85721-0065, USA

4. Department of Physics and Astronomy, University of Utah , Salt Lake City, UT 84112, USA

5. Department of Physics, University of Michigan , Ann Arbor, MI 48109, USA

6. Leinweber Center for Theoretical Physics, University of Michigan , Ann Arbor, MI 48109, USA

7. Department of Physics, Boise State University , Boise, ID 83725, USA

Abstract

ABSTRACT Within the ΛCDM cosmology, dark matter haloes are composed of both a smooth component and a population of smaller gravitationally bound subhaloes. These components are often treated as a single halo when properties, such as density profiles, are extracted from simulations. Recent work has shown that density profiles change substantially when subhalo mass is excluded. In this paper, we expand on this result by analysing three specific host halo properties – concentration (cNFW), spin (λB), and shape (c/a) – when calculated only from the smooth component of the halo. This analysis is performed on both Milky Way-mass haloes and cluster-mass haloes in high-resolution zoom-in N-body simulations. We find that when subhaloes are excluded, the median value of (1) cNFW is enhanced by $\approx 30\pm 11$ and $\approx 77\pm 8.1~{{\ \rm per\ cent}}$ for Milky Way-mass ($10^{12.1}\, \text{M}_\odot$) and cluster-mass ($10^{14.8}\, \text{M}_\odot$) haloes, respectively, (2) λB is reduced for Milky Way-mass by $\approx 11\pm 4.9~{{\ \rm per\ cent}}$ and cluster-mass haloes by $\approx 27\pm 3.5~{{\ \rm per\ cent}}$. Additionally, with the removal of subhaloes, cluster-mass haloes tend to become more spherical as the ratio of minor-to-major axis, c/a, increases by $\approx 11\pm 3.6~{{\ \rm per\ cent}}$, whereas Milky Way-mass haloes remain approximately the same shape with c/a changed by $\approx 1.0\pm 5.8~{{\ \rm per\ cent}}$. Fractional changes of each of these properties depend primarily on the amount of mass in subhaloes and, to a lesser extent, mass accretion history. Our findings demonstrate that the properties of the smooth components of dark matter haloes are biased relative to the total halo mass.

Funder

U.S. Department of Energy

University of Pittsburgh

University of Michigan

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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