Welcome to the new version of CaltechAUTHORS. Login is currently restricted to library staff. If you notice any issues, please email coda@library.caltech.edu
Published December 11, 2017 | Submitted + Accepted Version + Published
Journal Article Open

SIDM on fire: hydrodynamical self-interacting dark matter simulations of low-mass dwarf galaxies

Abstract

We compare a suite of four simulated dwarf galaxies formed in 10^(10)  M_⊙ haloes of collisionless cold dark matter (CDM) with galaxies simulated in the same haloes with an identical galaxy formation model but a non-zero cross-section for DM self-interactions. These cosmological zoom-in simulations are part of the Feedback In Realistic Environments (FIRE) project and utilize the FIRE-2 model for hydrodynamics and galaxy formation physics. We find the stellar masses of the galaxies formed in self-interacting dark matter (SIDM) with σ/m = 1 cm^2 g^(−1) are very similar to those in CDM (spanning M⋆ ≈ 10^(5.7–7.0)M_⊙) and all runs lie on a similar stellar mass–size relation. The logarithmic DM density slope (α = d log ρ/d log r) in the central 250-500pc remains steeper than α = −0.8 for the CDM-Hydro simulations with stellar mass M⋆ ∼ 10^(6.6) M_⊙ and core-like in the most massive galaxy. In contrast, every SIDM hydrodynamic simulation yields a flatter profile, with α > −0.4. Moreover, the central density profiles predicted in SIDM runs without baryons are similar to the SIDM runs that include FIRE-2 baryonic physics. Thus, SIDM appears to be much more robust to the inclusion of (potentially uncertain) baryonic physics than CDM on this mass scale, suggesting that SIDM will be easier to falsify than CDM using low-mass galaxies. Our FIRE simulations predict that galaxies less massive than M⋆ ≲ 3 × 10^6  M_⊙ provide potentially ideal targets for discriminating models, with SIDM producing substantial cores in such tiny galaxies and CDM producing cusps.

Additional Information

© 2017 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society. Accepted 2017 August 30. Received 2017 August 26; in original form 2017 June 16. Published: 05 September 2017. VHR acknowledges support from University of California Institute for Mexico and the United States (UC MEXUS) and Consejo Nacional de Ciencia y Tecnología (CONACyT) through the postdoctoral fellowship. AG-S acknowledges support from UC-MEXUS through the postdoctoral Fellowship. JSB and ODE are supported by National Science Foundation (NSF) AST-1518291, HST-AR-14282, HST-AR-13888 and NSF-PHY-1520921. MB-K acknowledges support from NSF grant AST-1517226 and from NASA grants NNX17AG29G and HST-AR-12836, HST-AR-13888, HST-AR-13896 and HST-AR-14282 from the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS5-26555. DK was supported by NSF grant AST-1412153 and the Cottrell Scholar Award from the Research Corporation for Science Advancement. C-AF-G was supported by NSF through grants AST-1412836 and AST-1517491, and by NASA through grant NNX15AB22G. Our simulations used computational resources provided via the NASA Advanced Supercomputing (NAS) Division and the NASA Center for Climate Simulation (NCCS) and the Extreme Science and Engineering Discovery Environment, which is supported by National Science Foundation grant number OCI-1053575.

Attached Files

Published - stx2253.pdf

Accepted Version - nihms-997014.pdf

Submitted - 1706.07514.pdf

Files

stx2253.pdf
Files (9.0 MB)
Name Size Download all
md5:00f372797cb72f2b72a1f553f6b4d246
2.3 MB Preview Download
md5:b704bcbb45ee8efa3324ee9640c97148
4.5 MB Preview Download
md5:16b32723ca690ed83c4324b29184e493
2.2 MB Preview Download

Additional details

Created:
August 19, 2023
Modified:
October 17, 2023