Because of the concerns just mentioned that CDM may predict higher densities and more substructure on small scales than is observed, many people have proposed alternatives to CDM. Two of these ideas that have been studied in the greatest detail are self-interacting dark matter (SIDM) [15] and warm dark matter (WDM).
Cold dark matter assumes that the dark matter particles have only weak interactions with each other and with other particles. SIDM assumes that the dark matter particles have strong elastic scattering cross sections, but negligible annihilation or dissipation. The hope was that SIDM might suppress the formation of the dense central regions of dark matter halos, although the large cross sections might also lead to high thermal conductivity which drains energy from halo centers and could lead to core collapse [109], and which also causes evaporation of galaxy halos in clusters, resulting in violation of the observed "fundamental plane" correlations [110]. But in any case, self-interaction cross sections large enough to have a significant effect on the centers of galaxy-mass halos will make the centers of galaxy clusters more spherical [111, 112] and perhaps also less dense [113, 114] than gravitational lensing observations [115] indicate.
Warm dark matter arises in particle physics theories in which the dark
matter particles have relatively high thermal velocities, for example
because their mass is
1 keV
[116],
comparable to the
temperature about a year after the Big Bang when the horizon first
encompassed the amount of dark matter in a large galaxy. Such a
velocity distribution can suppress the formation of structure on small
scales. Indeed, this leads to constraints on how low the WDM particle
mass can be. From the requirement that there is enough small-scale
power in the linear power spectrum to reproduce the observed
properties of the Ly
forest in quasar spectra, it follows that
this mass must exceed about 0.75 keV
[117].
The requirement
that there be enough small halos to host early galaxies to produce the
floor in metallicity observed in the
Ly
forest systems, and
early galaxies and quasars to reionize the universe, probably implies
a stronger lower limit on the WDM mass of at least 1 keV
[118].
Simulations [119,
120]
do show that there will be far fewer small satellite halos with
WDM than
CDM. However, as I
have already mentioned, inclusion of the
effects of reionization may make the observed numbers of satellite
galaxies consistent with the predictions of
CDM
[89],
in which case
WDM
may predict too few small satellite
galaxies. Lensing can be used to look for these
subhalos [121,
122]
and may already indicate that there are more of them than expected in
WDM
[123].
Thus it appears likely that WDM does not solve all the problems it was
invoked to solve, and may create new problems. Moreover, even with an
initial power spectrum truncated on small scales, simulations appear
to indicate that dark matter halos nevertheless have density profiles
much like those in CDM
[124,
68,
86]
(although doubts have been expressed about the reliability of such
simulations because of numerical relaxation
[125]).
But WDM does lead to lower
concentration halos in better agreement with observed rotation
velocity curves
[126,
127].
One theoretical direction that does appear very much worth
investigating is
CDM with a tilt
n ~ 0.9 in the primordial power spectrum
Pp(k)
kn
[128].
Such t
CDM
cosmology is favored by recent measurements of the power
spectrum of the Ly
forest
[36]
and appears to be
consistent with the latest CMB measurements and all other available
data [129].
Our simple analytic model
[61]
predicts that the concentration of halos in
t
CDM will be
approximately half that in LCDM, which appears to be true in a trial
simulation by A. Kravtsov. While this does not resolve the cusp
problem, it is a step in the right direction which may lessen the
conflict with galaxy rotation curves.