Cuspy dark matter density profiles in massive dwarf galaxies

Author:

Cooke Lauren H12ORCID,Levy Rebecca C13ORCID,Bolatto Alberto D1456ORCID,Simon Joshua D7ORCID,Newman Andrew B7ORCID,Teuben Peter1ORCID,Davey Brandon D18ORCID,Wright Melvyn9ORCID,Tarantino Elizabeth1ORCID,Lenkić Laura110ORCID,Villanueva Vicente1ORCID

Affiliation:

1. Department of Astronomy, University of Maryland , College Park, MD 20742, USA

2. Holton-Arms School , Bethesda, MD 20817, USA

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

4. Joint Space-Science Institute, University of Maryland , College Park, MD 20742, USA

5. Visiting Scholar, Flatiron Institute, Center for Computational Astrophysics , NY 10010, USA

6. Visiting Astronomer, National Radio Astronomy Observatory , VA 22903, USA

7. Observatories of the Carnegie Institution for Science , Pasadena, CA 91101, USA

8. Department of Physics, University of South Florida , Tampa, FL 33620, USA

9. Department of Astronomy, University of California , Berkeley, CA 94720, USA

10. SOFIA Science Center, USRA, NASA Ames Research Center , M.S. N232-12, Moffett Field, CA 94035, USA

Abstract

ABSTRACT Rotation curves of galaxies probe their total mass distributions, including dark matter. Dwarf galaxies are excellent systems to investigate the dark matter density distribution, as they tend to have larger fractions of dark matter compared to higher mass systems. The core-cusp problem describes the discrepancy found in the slope of the dark matter density profile in the centres of galaxies (β*) between observations of dwarf galaxies (shallower cores) and dark matter-only simulations (steeper cusps). We investigate β* in six nearby spiral dwarf galaxies for which high-resolution CO J = 1–0 data were obtained with ALMA (Atacama Large Millimeter/submillimeter Array). We derive rotation curves and decompose the mass profile of the dark matter using our CO rotation curves as a tracer of the total potential and 4.5 $\mu$m photometry to define the stellar mass distribution. We find 〈β*〉 = 0.6 with a standard deviation of ±0.1 among the galaxies in this sample, in agreement with previous measurements in this mass range. The galaxies studied are on the high stellar mass end of dwarf galaxies and have cuspier profiles than lower mass dwarfs, in agreement with other observations. When the same definition of the slope is used, we observe steeper slopes than predicted by the FIRE and NIHAO simulations. This may signal that these relatively massive dwarfs underwent stronger gas inflows towards their centres than predicted by these simulations, that these simulations overpredict the frequency of accretion or feedback events, or that a combination of these or other effects are at work.

Funder

University of Maryland

NSF

PIRE

AAG

ESO

NINS

NRC

NSC

KASI

NAOJ

National Radio Astronomy Observatory

Jet Propulsion Laboratory

California Institute of Technology

University of Hawaii

Johns Hopkins University

Durham University

University of Edinburgh

Queen's University Belfast

Harvard-Smithsonian Center for Astrophysics

Space Telescope Science Institute

National Aeronautics and Space Administration

Eotvos Lorand University

Los Alamos National Laboratory

Gordon and Betty Moore Foundation

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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