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Large-Scale Simulations of Reionization
Authors: Katharina
Kohler, Nickolay
Y. Gnedin, Andrew
J.S. Hamilton
Comments: 25 pages
We use cosmological simulations to explore the
large-scale effects of
reionization. Since reionization is a process that involves a large
dynamic
range - from galaxies to rare bright quasars - we need to be able to
cover a
significant volume of the universe in our simulation without losing hte
important small scale effects from galaxies. Here we have taken an
approach
that uses clumping factors derived from small scale simulations to
approximate
the radiative transfer on the sub-cell scales. Using this technique, we
can
cover a simulation size up to $1280 h^{-1} Mpc$ with $10 h^{-1} Mpc$
cells.
This allows us to construct synthetic spectra of quasars similar to
observed
spectra of SDSS quasars at high reshifts and compare them to the
observational
data. These spectra can then be analyzed for HII region sizes, the
presence of
the Gunn-Peterson trough and the Lyman-$\alpha$ forest.
Dark Matter Clumpiness
Cosmological Origin of Small-Scale Clumps and DM Annihilation
Signal
Authors: Veniamin
Berezinsky, Vyacheslav
Dokuchaev, Yury
Eroshenko
Comments: The new element of this paper is estimation of
contribution to annihilation from large-scale clumps in comparison with
small ones
Journal-ref: Proceedings of the 6th RESCEU International
Symposium on "Frontier in Astroparticle Physics and Cosmology", eds. K.
Sato and S. Nagataki (Universal Academy Press Inc.: Tokyo, Japan,
2004), p241-248
We study the cosmological origin of small-scale DM
clumps in the
hierarchical
scenario with the most conservative assumption of adiabatic Gaussian
fluctuations. The mass spectrum of small-scale clumps with
M<10^3Msun is
calculated with tidal destruction of the clumps taken into account
within the
hierarchical model of clump structure. Only 0.1-0.5% of small clumps
survive
the stage of tidal destruction in each logarithmic mass interval. The
mass
distribution of clumps has a cutoff at Mmin due to diffusion of DM
particles
out of a fluctuation and free streaming at later stage. Mmin is a model
dependent quantity. In the case the neutralino DM, considered as a pure
bino,
Mmin~10^-8 Msun. The evolution of density profile in a DM clump does
not result
in the singularity because of formation of the core under influence of
tidal
interaction. The radius of the core is ~0.1R, where R is radius of the
clump.
The applications for annihilation of DM particles in the Galactic halo
are
studied. The number density of clumps as a function of their mass,
radius and
distance to the Galactic center is presented. The enhancement of
annihilation
signal due to clumpiness, valid for arbitrary DM particles, is
calculated. In
spite of small survival probability, the global annihilation signal in
most
cases is dominated by clumps, with major contribution given by small
clumps.
The enhancement due to large clumps with M>10^6 Msun is very small.
DM clumps as discrete sources of gamma-radiation
Authors: K.M.
Belotsky, A.M.
Galper
Comments: 4 pages, 2 figures
Massive objects (clumps) of Cold Dark Matter (CDM) in
Galaxy can appear
due
to its annihilation as discrete sources of gamma-radiation. Some number
of
unidentified regular gamma-sources, observed by EGRET, can be accounted
for by
massive CDM clumps. Future gamma-ray expreriment GLAST in combination
with data
of EGRET will enable to probe a wide range of models of clumped
annihilating
CDM.
Earth-mass dark-matter haloes as the first structures in the
early Universe
Authors: Juerg
Diemand, Ben
Moore, Joachim
Stadel (University of Zurich)
Comments: 11 pages, 3 figures, published in Nature,
January 27, 2005
Subj-class: Astrophysics; Space Physics
Journal-ref: Nature 433 (2005) 389-391
The Universe was nearly smooth and homogeneous before
a redshift of z =
100,
about 20 million years after the Big Bang. After this epoch, the tiny
fluctuations imprinted upon the matter distribution during the initial
expansion began to collapse because of gravity. The properties of these
fluctuations depend on the unknown nature of dark matter, the
determination of
which is one of the biggest challenges in present-day science. Here we
report
supercomputer simulations of the concordance cosmological model, which
assumes
neutralino dark matter (at present the preferred candidate), and find
that the
first objects to form are numerous Earth-mass dark-matter haloes about
as large
as the Solar System. They are stable against gravitational disruption,
even
within the central regions of the Milky Way. We expect over 10^15 to
survive
within the Galactic halo, with one passing through the Solar System
every few
thousand years. The nearest structures should be among the brightest
sources of
gamma-rays (from particle-particle annihilation).
Indications for a preferred reference frame from an
ether-drift experiment
Authors: M.
Consoli, E.
Costanzo
Comments: 7 pages, plain Latex
We present a fully model-independent analysis of the
extensive
observations
reported by a recent ether-drift experiment in Berlin. No a priori
assumption
is made on the nature of a hypothetical preferred frame. We find a
remarkable
consistency with an Earth's cosmic motion exhibiting an average
declination
angle |\gamma|\sim 43^o and with values of the RMS anisotropy parameter
(1/2-\beta+\delta) that are one order of magnitude larger than the
presently
quoted ones. This might represent the first modern indication for a
preferred
frame and for a non-zero anisotropy of the speed of light.
A Gravitational Tractor for Towing Asteroids
Authors: Edward
T. Lu, Stanley
G. Love
Comments: 4 pages, 1 figure - to be published in Nature
We present a concept for a spacecraft that can controllably alter the
trajectory of an Earth threatening asteroid using gravity as a towline.
The
spacecraft hovers near the asteroid with thrusters angled outward so
the
exhaust does not impinge on the surface. This deflection method is
insensitive
to the structure, surface properties, and rotation state of the
asteroid.
Producing a Scale-Invariant Spectrum of Perturbations in a
Hagedorn Phase of String Cosmology
Authors: Ali
Nayeri, Robert
H. Brandenberger, Cumrun
Vafa
Comments: 4 pages, 1 figure
Report-no: HUTP-05/A048
We study the generation of cosmological perturbations
during the
Hagedorn
phase of string gas cosmology. Using tools of string thermodynamics we
provide
indications that it may be possible to obtain a nearly scale-invariant
spectrum
of cosmological fluctuations on scales which are of cosmological
interest
today. In our cosmological scenario, the early Hagedorn phase of string
gas
cosmology goes over smoothly into the radiation-dominated phase of
standard
cosmology, without having a period of cosmological inflation.
Dimensionless constants, cosmology and other dark matters
Authors: Max
Tegmark (MIT), Anthony
Aguirre (UCSC), Martin
Rees (Cambridge), Frank
Wilczek (MIT)
Comments: 29 pages, 12 figs
We identify 31 dimensionless physical constants
required by particle
physics
and cosmology, and emphasize that both microphysical constraints and
selection
effects might help elucidate their origin. Axion cosmology provides an
instructive example, in which these two kinds of arguments must both be
taken
into account, and work well together. If a Peccei-Quinn phase
transition
occurred before or during inflation, then the axion dark matter density
will
vary from place to place with a probability distribution. By
calculating the
net dark matter halo formation rate as a function of all four relevant
cosmological parameters and assessing other constraints, we find that
this
probability distribution, computed at stable solar systems, is arguably
peaked
near the observed dark matter density. If cosmologically relevant WIMP
dark
matter is discovered, then one naturally expects comparable densities
of WIMPs
and axions, making it important to follow up with precision
measurements to
determine whether WIMPs account for all of the dark matter or merely
part of
it.
Probing neutrino masses with CMB lensing extraction
Authors: Julien
Lesgourgues, Laurence
Perotto, Sergio
Pastor, Michel
Piat
Comments: 13 pages, 3 figures
Report-no: LAPTH-1128/05, IFIC/05-60, APC-05-90
We evaluate the ability of future cosmic microwave
background (CMB)
experiments to measure the power spectrum of large scale structure
using
quadratic estimators of the weak lensing deflection field. We calculate
the
sensitivity of upcoming CMB experiments such as BICEP, QUaD, BRAIN,
ClOVER and
PLANCK to the non-zero total neutrino mass M_nu indicated by current
neutrino
oscillation data. We find that these experiments greatly benefit from
lensing
extraction techniques, improving their one-sigma sensitivity to M_nu by
a
factor of order four. The combination of data from PLANCK and the
SAMPAN
mini-satellite project would lead to sigma(M_nu) = 0.1 eV, while a
value as
small as sigma(M_nu) = 0.035 eV is within the reach of a space mission
based on
bolometers with a passively cooled 3-4 m aperture telescope,
representative of
the most ambitious projects currently under investigation. We show that
our
results are robust not only considering possible difficulties in
subtracting
astrophysical foregrounds from the primary CMB signal but also when the
minimal
cosmological model (Lambda Mixed Dark Matter) is generalized in order
to
include a possible scalar tilt running, a constant equation of state
parameter
for the dark energy and/or extra relativistic degrees of freedom.
Inflation at the TeV scale with a PNGB curvaton
Authors: Konstantinos
Dimopoulos
Comments: 14 pages, 1 figure
We investigate a particular type of curvaton
mechanism, under which
inflation
can occur at Hubble scale of order 1 TeV. The curvaton is a pseudo
Nambu-Goldstone boson, whose order parameter increases after a phase
transition
during inflation, triggered by the gradual decrease of the Hubble
scale. The
mechanism is studied in the context of modular inflation, where the
inflaton is
a string axion. We show that the mechanism is successful for natural
values of
the model parameters, provided the phase transition occurs much earlier
than
the time when the cosmological scales exit the horizon. Also, it turns
our that
the radial mode for our curvaton must be a flaton field.
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