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Published September 2021 | Submitted + Published
Journal Article Open

Dissipative dark matter on FIRE – I. Structural and kinematic properties of dwarf galaxies

Abstract

We present the first set of cosmological baryonic zoom-in simulations of galaxies including dissipative self-interacting dark matter (dSIDM). These simulations utilize the Feedback In Realistic Environments galaxy formation physics, but allow the dark matter to have dissipative self-interactions analogous to standard model forces, parametrized by the self-interaction cross-section per unit mass, (σ/m), and the dimensionless degree of dissipation, 0 < f_(diss) < 1. We survey this parameter space, including constant and velocity-dependent cross-sections, and focus on structural and kinematic properties of dwarf galaxies with M_(halo)∼10¹⁰⁻¹¹ M⊙ and M∗∼10⁵⁻⁸ M⊙. Central density profiles (parametrized as ρ ∝ rα) of simulated dwarfs become cuspy when (σ/m)_(eff) ≳ 0.1cm²g⁻¹ (and f_(diss) = 0.5 as fiducial). The power-law slopes asymptote to α ≈ −1.5 in low-mass dwarfs independent of cross-section, which arises from a dark matter 'cooling flow'. Through comparisons with dark matter only simulations, we find the profile in this regime is insensitive to the inclusion of baryons. However, when (σ/m)_(eff) ≪ 0.1cm²g⁻¹⁠, baryonic effects can produce cored density profiles comparable to non-dissipative cold dark matter (CDM) runs but at smaller radii. Simulated galaxies with (σ/m) ≳ 10cm²g⁻¹ and the fiducial f_(diss) develop significant coherent rotation of dark matter, accompanied by halo deformation, but this is unlike the well-defined thin 'dark discs' often attributed to baryon-like dSIDM. The density profiles in this high cross-section model exhibit lower normalizations given the onset of halo deformation. For our surveyed dSIDM parameters, halo masses and galaxy stellar masses do not show appreciable difference from CDM, but dark matter kinematics and halo concentrations/shapes can differ.

Additional Information

© 2021 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society. This article is published and distributed under the terms of the Oxford University Press, Standard Journals Publication Model (https://academic.oup.com/journals/pages/open_access/funder_policies/chorus/standard_publication_model). Accepted 2021 July 6. Received 2021 July 2; in original form 2021 February 18. Published: 19 July 2021. Support for PFH was provided by the National Science Foundation (NSF) research grants 1911233 and 20009234, NSF Faculty Early Career Development Program (CAREER) grant 1455342, and the National Aeronautics and Space Administration (NASA) grants 80NSSC18K0562 and HST-AR-15800.001-A. Numerical calculations were run on the Caltech compute cluster 'Wheeler', allocations FTA-Hopkins/AST20016 supported by the NSF and the Texas Advanced Computing Center (TACC), and NASA HEC SMD-16-7592. LN is supported by the United States Department of Energy (DOE) under Award Number DESC0011632, the Sherman Fairchild Foundation fellowship, the University of California Presidential fellowship, and the fellowship of theoretical astrophysics at Carnegie Observatories. FJ is supported by the Troesh scholarship. MBK acknowledges support from NSF CAREER award AST-1752913, NSF grant AST-1910346, NASA grant NNX17AG29G, and HST-AR-15006, HST-AR-15809, HST-GO-15658, HST-GO-15901, HST-GO-15902, HST-AR-16159, and HST-GO-16226 from the Space Telescope Science Institute (STScI), which is operated by the Association of Universities for Research in Astronomy (AURA), Inc., under NASA contract NAS5-26555. AW received support from NASA through the Astrophysics Theory Program (ATP) grants 80NSSC18K1097 and 80NSSC20K0513; the Hubble Space Telescope (HST) grants GO-14734, AR-15057, AR-15809, and GO-15902 from STScI; a Scialog Award from the Heising-Simons Foundation; and a Hellman Fellowship. Data Availability: The simulation data of this work were generated and stored on the supercomputing system Frontera at the Texas Advanced Computing Center (TACC), under the allocations FTA-Hopkins/AST20016 supported by the NSF and TACC, and NASA HEC SMD-16-7592. The data underlying this article cannot be shared publicly immediately, since the series of paper is still in development. The data will be shared on reasonable request to the corresponding author.

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Additional details

Created:
August 20, 2023
Modified:
October 23, 2023