Abstract:
JCAP04(2016)012
ou
rnal of
C
osmology and
A
strop
article
P
hysics
An IOP and SISSA journal
J
The effects of the small-scale DM
power on the cosmological neutral
hydrogen (H
i
) distribution at high
redshifts
Abir Sarkar,
a,b
Rajesh Mondal,
c,d
Subinoy Das,
e
Shiv.K. Sethi,
a
Somnath Bharadwaj
c,d
and David J.E. Marsh
f
a
Department of Astronomy And Astrophysics, Raman Research Institue,
C.V. Raman Avenue, Bangalore, India
b
Department of Physics, Indian Institue of Science,
C.V. Raman Avenue, Bangalore, India
c
Department of Physics, Indian Institute of Technology Kharagpur,
Kharagpur 721302, India
d
Centre for Theoretical Studies, Indian Institute of Technology Kharagpur,
Kharagpur 721302, India
e
Indian Institue of Astrophysics,
100 Feet Rd, Madiwala, Bangalore, India
f
Department of Physics, King’s College London,
Strand, London, WC2R 2LS, United Kingdom
E-mail: abir@rri.res.in, rm@phy.iitkgp.ernet.in, subinoy@iiap.res.in,
sethi@rri.res.in, somnath@phy.iitkgp.ernet.in, david.marsh@kcl.ac.uk
Received December 17, 2015
Revised February 24, 2016
Accepted March 29, 2016
Published April 7, 2016
Abstract.
The particle nature of dark matter remains a mystery. In this paper, we consider
two dark matter models — Late Forming Dark Matter (LFDM) and Ultra-Light Axion
(ULA) models — where the matter power spectra show novel effects on small scales. The
high redshift universe offers a powerful probe of their parameters. In particular, we study two
cosmological observables: the neutral hydrogen (HI) redshifted 21-cm signal from the epoch of
reionization, and the evolution of the collapsed fraction of HI in the redshift range 2
< z <
5.
We model the theoretical predictions of the models using CDM-like N-body simulations with
modified initial conditions, and generate reionization fields using an excursion set model.
The N-body approximation is valid on the length and halo mass scales studied. We show
that LFDM and ULA models predict an increase in the HI power spectrum from the epoch JCAP04(2016)012
of reionization by a factor between 2–10 for a range of scales 0
.
1
< k <
4 Mpc
−
1
. Assuming
a fiducial model where a neutral hydrogen fraction ̄
x
HI
= 0
.
5 must be achieved by
z
= 8,
the reionization process allows us to put approximate bounds on the redshift of dark matter
formation
z
f
>
4
×
10
5
(for LFDM) and the axion mass
m
a
>
2
.
6
×
10
−
23
eV (for ULA).
The comparison of the collapsed mass fraction inferred from damped Lyman-
α
observations
to the theoretical predictions of our models lead to the weaker bounds:
z
f
>
2
×
10
5
and
m
a
>
10
−
23
eV. These bounds are consistent with other constraints in the literature using
different observables; we briefly discuss how these bounds compare with possible constraints
from the observation of luminosity function of galaxies at high redshifts. In the case of ULAs,
these constraints are also consistent with a solution to the cusp-core problem of CDM.