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COZMIC. I. Cosmological Zoom-in Simulations with Initial Conditions Beyond Cold Dark Matter
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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.
American Astronomical Society
Title: COZMIC. I. Cosmological Zoom-in Simulations with Initial Conditions Beyond Cold Dark Matter
Description:
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.
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