958 research outputs found
Missing Power vs low-l Alignments in the Cosmic Microwave Background: No Correlation in the Standard Cosmological Model
On large angular scales (greater than about 60 degrees), the two-point
angular correlation function of the temperature of the cosmic microwave
background (CMB), as measured (outside of the plane of the Galaxy) by the
Wilkinson Microwave Anisotropy Probe, shows significantly lower large-angle
correlations than expected from the standard inflationary cosmological model.
Furthermore, when derived from the full CMB sky, the two lowest cosmologically
interesting multipoles, the quadrupole (l=2) and the octopole (l=3), are
unexpectedly aligned with each other. Using randomly generated full-sky and
cut-sky maps, we investigate whether these anomalies are correlated at a
statistically significant level. We conclusively demonstrate that, assuming
Gaussian random and statistically isotropic CMB anisotropies, there is no
statistically significant correlation between the missing power on large
angular scales in the CMB and the alignment of the l=2 and l=3 multipoles. The
chance to measure the sky with both such a lack of large-angle correlation and
such an alignment of the low multipoles is thus quantified to be below 10^{-6}.Comment: 4 Pages, 1 Figur
Quasars and galaxy formation
Quasars are widely believed to be powered by accretion onto supermassive
black holes and there is now considerable evidence for a link between mergers,
quasars and the formation of spheroids. Cattaneo, Haehnelt & Rees (1999) have
demonstrated that a very simple model in which supermassive black holes form
and accrete most of their mass in mergers of galaxies of comparable masses can
reproduce the observed relation of black hole mass to bulge luminosity. Here we
show that this simple model can account for the luminosity function of quasars
and for the redshift evolution of the quasar population provided a few
additional assumptions are made. We use the extended Press-Schechter formalism
to simulate the formation of galaxies in hierarchical models of the formation
of structures and we assume that, when two galaxies of comparable masses merge,
their central black holes coalesce and a fraction of the gas in the merger
remnant is accreted by the supermassive black hole over a time-scale of about
10^7 yr. We find that the decrease in the merging rate with cosmic time and the
depletion in the amount of cold gas available due to the formation of stars are
not sufficient to explain the strong decline in the space density of bright
quasars between z=2 and z=0, since larger and larger structures form, which can
potentially host brighter and brighter quasars. To explain the redshift
evolution of the space density of bright quasars between z=2 and z=0 we need to
assume that there is a dependence on redshift either in the fraction of
available gas accreted or in the time-scale for accretion.Comment: 8 pages, 8 figures, submitted to MNRA
Can one reconstruct masked CMB sky?
The CMB maps obtained by observations always possess domains which have to be
masked due to severe uncertainties with respect to the genuine CMB signal.
Cosmological analyses ideally use full CMB maps in order to get e.g. the
angular power spectrum. There are attempts to reconstruct the masked regions at
least at low resolutions, i.e. at large angular scales, before a further
analysis follows. In this paper, the quality of the reconstruction is
investigated for the ILC (7yr) map as well as for 1000 CMB simulations of the
LambdaCDM concordance model. The latter allows an error estimation for the
reconstruction algorithm which reveals some drawbacks. The analysis points to
errors of the order of a significant fraction of the mean temperature
fluctuation of the CMB. The temperature 2-point correlation function C(theta)
is evaluated for different reconstructed sky maps which leads to the conclusion
that it is safest to compute it on the cut-sky
Low-frequency line temperatures of the CMB
Based on SU(2) Yang-Mills thermodynamics we interprete Aracde2's and the
results of earlier radio-surveys on low-frequency CMB line temperatures as a
phase-boundary effect. We explain the excess at low frequencies by evanescent,
nonthermal photon fields of the CMB whose intensity is nulled by that of Planck
distributed calibrator photons. The CMB baseline temperature thus is identified
with the critical temperature of the deconfining-preconfining transition.Comment: v2: 9 pages, 1 figure, extended discussion of why prsent photon mass
bounds are not in contradiction to a low-temperature, low-frequency Meissner
mass responsible for UEGE, matches journal versio
Angular Signatures for Galactic Halo WIMP Scattering in Direct Detectors: Prospects and Challenges
Angular Sensitivity can provide a key additional tool which might allow
unambiguous separation of a signal due to Galactic halo WIMPs from other
possible backgrounds in direct detectors. We provide a formalism which allows a
calculation of the expected angular distribution of events in terrestrial
detectors with angular sensitivity for any incident distribution of Galactic
halo dark matter. This can be used as an input when studying the sensitivity of
specific detectors to halo WIMPs. We utilize this formalism to examine the
expected signature for WIMP dark matter using a variety of existing analytic
halo models in order to explore how uncertainty in the Galactic halo
distribution impact on the the event rates that may be required to separate a
possible WIMP signal from other terrestrial backgrounds. We find that as few as
30 events might be required to disentangle the signal from backgrounds if the
WIMP distribution resembles an isothermal sphere distribution. On the other
hand, for certain halo distributions, even detectors with fine scale resolution
may require in excess of a 100-400 events to distinguish a WIMP signal from
backgrounds using angular sensitivity. We also note that for finite thresholds
the different energy dependence of spin-dependent scattering cross sections may
require a greater number of events to discern a WIMP signal than for spin
independent interactions. Finally, we briefly describe ongoing studies aimed at
developing strategies to better exploit angular signatures, and the use of
N-body simulations to better model the expected halo distribution in predicting
the expected signature for direct WIMP detectors.Comment: 21 pages latex, including 16 figures. Submitted to Phys. Rev.
Pre-Heated Isentropic Gas in Groups of Galaxies
We confirm that the standard assumption of isothermal, shock-heated gas in
cluster potentials is unable to reproduce the observed X-ray luminosity-
temperature relation of groups of galaxies. As an alternative, we construct a
physically motivated model for the adiabatic collapse of pre-heated gas into an
isothermal potential that improves upon the original work of Kaiser (1991). The
luminosity and temperature of the gas is calculated, assuming an appropriate
distribution of halo formation times and radiation due to both bremsstrahlung
and recombination processes. This model successfully reproduces the slope and
dispersion of the luminosity-temperature relation of galaxy groups. We also
present calculations of the temperature and luminosity functions for galaxy
groups under the prescription of this model. This model makes two strong
predictions for haloes with total masses M<10^13 M_sun, which are not yet
testable with current data: (1) the gas mass fraction will increase in direct
proportion to the halo mass; (2) the gas temperature will be larger than the
virial temperature of the mass. The second effect is strong enough that group
masses determined from gas temperatures will be overestimated by about an order
of magnitude if it is assumed that the gas temperature is the virial
temperature. The entropy required to match observations can be obtained by
heating the gas at the turnaround time, for example, to about 3 X 10^6 K at
z=1, which is too high to be generated by a normal rate of supernova
explosions. This model breaks down on the scale of low mass clusters, but this
is an acceptable limitation, as we expect accretion shocks to contribute
significantly to the entropy of the gas in such objects.Comment: Final, refereed version, accepted by MNRAS. One new figure and
several clarifying statements have been added. Uses mn.a4.sty (hacked
mn.sty). Also available from
http://astrowww.phys.uvic.ca/~balogh/entropy.ps.g
Large-angle anomalies in the CMB
We review the recently found large-scale anomalies in the maps of temperature
anisotropies in the cosmic microwave background. These include alignments of
the largest modes of CMB anisotropy with each other and with geometry and
direction of motion of the Solar System, and the unusually low power at these
largest scales. We discuss these findings in relation to expectation from
standard inflationary cosmology, their statistical significance, the tools to
study them, and the various attempts to explain them.Comment: Review in the Advances in Astronomy special issue "Testing the
Gaussianity and Statistical Isotropy of the Universe" (eds. D. Huterer, E.
Komatsu and S. Shandera); 16 pages, 7 figures. v2 matches the published
versio
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