COZMIC. I. Cosmological Zoom-in Simulations with Initial Conditions Beyond Cold Dark Matter
Ethan O. Nadler, Rui An, Vera Gluscevic, Andrew Benson, Xiaolong Du
Abstract
Abstract We present 72 cosmological dark-matter--only N -body zoom-in simulations with initial conditions beyond cold, collisionless dark matter (CDM), as the first installment of the COZMIC suite. We simulate Milky Way (MW) analogs with linear matter power spectra P ( k ) for (i) thermal-relic warm dark matter (WDM) with masses m WDM ∈ [3, 4, 5, 6, 6.5, 10]keV, (ii) fuzzy dark matter (FDM) with masses m FDM ∈ [25.9,69.4, 113, 151, 185, 490] × 10 −22 eV, and (iii) interacting dark matter (IDM) with a velocity-dependent elastic proton scattering cross section σ = σ 0 v n , relative particle velocity scaling n ∈ [2, 4], and dark matter mass m IDM ∈ [10 −4 , 10 −2 , 1] GeV. Subhalo mass function (SHMF) suppression is significantly steeper in FDM versus WDM, while dark acoustic oscillations in P ( k ) can reduce SHMF suppression for IDM. We fit SHMF models to our simulation results and derive new bounds on WDM and FDM from the MW satellite population, obtaining m WDM > 5.9 keV and m FDM > 1.4 × 10 −20 eV at 95% confidence; these limits are ≈10% weaker and 5× stronger than previous constraints owing to the updated transfer functions and SHMF models, respectively. We estimate IDM bounds for n = 2 ( n = 4) and obtain σ 0 < 1.0 × 10 −27 cm 2 , 1.3 × 10 −24 cm 2 , and 3.1 × 10 −23 cm 2 ( σ 0 < 9.9 × 10 −27 cm 2 , 9.8 × 10 −21 cm 2 , and 2.1 × 10 −17 cm 2 ) for m IDM = 10 −4 , 10 −2 , and 1 GeV, respectively. Thus, future development of IDM SHMF models can improve IDM cross section bounds by up to a factor of ∼20 with current data. COZMIC presents an important step toward accurate small-scale structure modeling in beyond-CDM cosmologies, critical to upcoming observational searches for dark matter physics.