Monday, January 17, 2011
arXiv: 17 January 2011
Thursday, January 13, 2011
arXiv: 14 January 2011
Testing a Phenomenologically Extended DGP Model with Upcoming Weak Lensing Surveys
Properties of the HII region populations of M51 and NGC 4449 from Halpha images with ACS on HST
Growth factor and galaxy bias from future redshift surveys: a study on parametrizations
Towards a Cosmological Dual to Inflation
Wednesday, January 12, 2011
arXiv: 13 January 2011
Cosmological magnetic field survival
HST/NICMOS Imaging of Bright High-Redshift 24μm-selected Galaxies: Merging Properties
Are small-scale sub-structures a universal property of galaxy halos? The case of the giant elliptical NGC~5128
arXiv: 12 January 2010
Marvin Weinstein
http://arxiv.org/abs/1101.2177v1
This paper makes the simple observation that a fundamental length, or
cutoff, in the context of Friedmann-Lema\^itre-Robertson-Walker (FRW)
cosmology implies very different things than for a static universe. It
is argued that it is reasonable to assume that this cutoff is
implemented by fixing the number of quantum degrees of freedom per
co-moving volume (as opposed to a Planck volume) and the relationship
of the vacuum-energy of all of the fields in the theory to the
cosmological constant (or dark energy) is re-examined. The
restrictions that need to be satisfied by a generic theory to avoid
conflicts with current experiments are discussed, and it is shown that
in any theory satisfying these constraints knowing the difference
between $w$ and minus one allows one to predict $\dot{w}$. It is
argued that this is a robust result and if this prediction fails the
idea of a fundamental cutoff of the type being discussed can be ruled
out. Finally, it is observed that, within the context of a specific
theory, a co-moving cutoff implies a predictable time variation of
fundamental constants. This is accompanied by a general discussion of
why this is so, what are the strongest phenomenological limits upon
this predicted variation, and which limits are in tension with the
idea of a co-moving cutoff. It is pointed out, however, that a careful
comparison of the predicted time variation of fundamental constants is
not possible without restricting to a particular model field-theory
and that is not done in this paper.
The Cosmogrid Simulation: Statistical Properties of Small Dark Matter Halos
Tomoaki Ishiyama, Junichiro Makino, Simon Portegies Zwart, Derek
Groen, Keigo Nitadori, Steven Rieder, Cees de Laat, Stephen McMillan,
Kei Hiraki, Stefan Harfst
http://arxiv.org/abs/1101.2020v1
We present the results of the "Cosmogrid" cosmological N-body
simulation suites based on the concordance LCDM model. The Cosmogrid
simulation was performed in a 30Mpc box with 2048^3 particles. The
mass of each particle is 1.28x10^5 Msun which is sufficient to resolve
ultra-faint dwarfs. We found that the halo mass function shows good
agreement with the Sheth and Tormen (1999) fitting function down to
~10^7 Msun. We have analyzed the spherically averaged density profiles
of the three most massive halos which are of galaxy group size and
contain at least 170 million particles. The slopes of these density
profiles become shallower than -1 at the inner most radius. We also
find a clear correlation of halo concentration with mass. The mass
dependence of the concentration parameter cannot be expressed by a
single power law, however a simple model based on the Press-Schechter
theory gives reasonable agreement with this dependence. The spin
parameter does not show a correlation with the halo mass. The
probability distribution functions for both concentration and spin are
well fitted by the log-normal distribution for halos with the masses
larger than ~10^8 Msun.
Planck Early Results: The Power Spectrum Of Cosmic Infrared Background
Anisotropies
Planck Collaboration: P. A. R. Ade, N. Aghanim, M. Arnaud, M. Ashdown,
J. Aumont, C. Baccigalupi, A. Balbi, A. J. Banday, R. B. Barreiro, J.
G. Bartlett, E. Battaner, K. Benabed, A. Benoit, J.-P. Bernard, M.
Bersanelli, R. Bhatia, K. Blagrave, J. J. Bock, A. Bonaldi, L.
Bonavera, J. R. Bond, J. Borrill, F. R. Bouchet, M. Bucher, C.
Burigana, P. Cabella, J.-F. Cardoso, A. Catalano, L. Cayon, A.
Challinor, A. Chamballu, L.-Y Chiang, C. Chiang, P. R. Christensen, D.
L. Clements, S. Colombi, F. Couchot, A. Coulais, B. P. Crill, F.
Cuttaia, L. Danese, R. D. Davies, R. J. Davis, P. de Bernardis, G. de
Gasperis, A. de Rosa, G. de Zotti, J. Delabrouille, J.-M. Delouis,
F.-X. Desert, H. Dole, S. Donzelli, O. Dore, U. Dorl, M. Douspis, X.
Dupac, G. Efstathiou, T. A. Ensslin, H. K. Eriksen, F. Finelli,
et al. (144 additional authors not shown)
http://arxiv.org/abs/1101.2028v1
Using Planck maps of six regions of low Galactic dust emission with a
total area of about 140 square degrees, we determine the angular power
spectra of Cosmic Infrared Background (CIB) anisotropies from
multipole l = 200 to l = 2000 at 217, 353, 545 and 857 GHz. We use
observations of HI emission as a tracer of thermal dust emission in
order to reduce the already low level of Galactic dust emission and
use the 143 GHz Planck maps in these fields to clean out cosmic
microwave background anisotropies. Both of these cleaning processes
are necessary in order to avoid significant contamination of the CIB
signal. We measure correlated CIB structure across frequencies. As
expected, the correlation decreases with increasing frequency
separation as the contribution of high-redshift galaxies to CIB
anisotropies increases with wavelengths. We find no significant
difference between the frequency spectrum of the CIB anisotropies and
the CIB mean, with dI/I=15% from 217 to 857 GHz. In terms of
clustering properties, the Planck data alone ruled out the linear
scale- and redshift- independent bias model. Non-linear corrections
are important. Consequently, we develop an alternative model that
couples a dusty galaxy, parametric evolution model with a simple halo
model approach. It provides an excellent fit to the measured
anisotropy angular power spectra and suggests that a different halo
occupation distribution is required at each frequency, which is
consistent with the fact that we expect each frequency to be dominated
by contributions from different redshifts. In our best-fit model, half
of the anisotropies power at l=2000 comes from redshifts z<0.8 at 857
GHz and z<0.9 at 545 GHz, while about 1/5 and 2/3 come from redshifts
z>3.5 at 353 and 217 GHz, respectively.
A Deep Dive into f(R) Gravity Theory
Solmaz Asgari, Reza Saffari
http://arxiv.org/abs/1101.2132v1
In this paper we derive behavior of deceleration parameter with
respect to redshift in context of f(R) gravity in vacuum. Here we show
that f(R) gravity will cover all the dynamical history of the Universe
from the beginning to the late time accelerating phase transition.
Here we obtained a continues inflationary behavior of the Universe
before the main inflationary period.
arXiv: 11 January 2010
J. W. Moffat
http://arxiv.org/abs/1101.1935v1
Modified Gravity (MOG) has been used successfully to explain the
rotation curves of galaxies, the motion of galaxy clusters, the Bullet
Cluster, and cosmological observations without the use of dark matter
or Einstein's cosmological constant. We review the main theoretical
ideas and applications of the theory to astrophysical and cosmological
data.
The Atacama Cosmology Telescope: Detection of Sunyaev-Zel'dovich
Decrement in Groups and Clusters Associated with Luminous Red Galaxies
Nick Hand, John William Appel, Nick Battaglia, J Richard Bond, Sudeep
Das, Mark J. Devlin, Joanna Dunkley, Rolando Dunner, Thomas
Essinger-Hileman, Joseph W. Fowler, Amir Hajian, Mark Halpern, Matthew
Hasselfield, Matt Hilton, Adam D. Hincks, Renee Hlozek, John P.
Hughes, Kent D. Irwin, Jeff Klein, Arthur Kosowsky, Yen-Ting Lin,
Tobias A. Marriage, Danica Marsden, Mike McLaren, Felipe Menanteau,
Kavilan Moodley, Michael D. Niemack, Michael R. Nolta, Lyman A. Page,
Lucas Parker, Bruce Partridge, Reed Plimpton, Erik D. Reese, Felipe
Rojas, Neelima Sehgal, Blake D. Sherwin, Jonathan L. Sievers, David N.
Spergel, Suzanne T. Staggs, Daniel S. Swetz, Eric R. Switzer, Robert
Thornton, Hy Trac, Katerina Visnjic, Ed Wollack
http://arxiv.org/abs/1101.1951v1
We present a detection of the Sunyaev-Zel'dovich (SZ) decrement
associated with the Luminous Red Galaxy (LRG) sample of the Sloan
Digital Sky Survey. The SZ data come from 148 GHz maps of the
equatorial region made by the Atacama Cosmology Telescope (ACT). The
LRG sample is divided by luminosity into four bins, and estimates for
the central Sunyaev-Zel'dovich (SZ) temperature decrement are
calculated through a stacking process. We detect and account for a
bias of the SZ signal due to weak radio sources. We use numerical
simulations to relate the observed decrement to Y200 and clustering
properties to relate the galaxy luminosity bins to mass. We also use a
relation between BCG luminosity and cluster mass based on stacked
gravitational lensing measurements to estimate the characteristic halo
masses. The masses are found to be in the range 1e13 - 1e14 M_sun, a
lower range than has been previously probed.
Exploring a string-like landscape
Jonathan Frazer, Andrew R Liddle
http://arxiv.org/abs/1101.1619v1
We explore inflationary trajectories within randomly-generated
two-dimensional potentials, considered as a toy model of the string
landscape. Both the background and perturbation equations are solved
numerically, the latter using the two-field formalism of Peterson and
Tegmark which fully incorporates the effect of isocurvature
perturbations. Sufficient inflation is a rare event, occurring for
only roughly one in $10^5$ potentials. For models generating
sufficient inflation, we find that the majority of runs satisfy
current constraints from WMAP. The scalar spectral index is less than
1 in all runs. The tensor-to-scalar ratio is below the current limit,
while typically large enough to be detected by next-generation CMB
experiments and perhaps also by Planck. In many cases the inflationary
consistency equation is broken by the effect of isocurvature modes.
Robustness to systematics for future dark energy probes
M. C. March (Imperial), R. Trotta (Imperial), L. Amendola
(Heidelberg), D. Huterer (U. of Michigan)
http://arxiv.org/abs/1101.1521v1
We extend the Figure of Merit formalism usually adopted to quantify
the statistical performance of future dark energy probes to assess the
robustness of a future mission to plausible systematic bias. We
introduce a new robustness Figure of Merit which can be computed in
the Fisher Matrix formalism given arbitrary systematic biases in the
observable quantities. We argue that robustness to systematics is an
important new quantity that should be taken into account when
optimizing future surveys. We illustrate our formalism with toy
examples, and apply it to future type Ia supernova (SNIa) and baryonic
acoustic oscillation (BAO) surveys. For the simplified systematic
biases that we consider, we find that SNIa are a somewhat more robust
probe of dark energy parameters than the BAO. We trace this back to a
geometrical alignement of systematic bias direction with statistical
degeneracy directions in the dark energy parameter space.
Extension of loop quantum gravity to $f(R)$ theories
Xiangdong Zhang, Yongge Ma
http://arxiv.org/abs/1101.1752v1
The 4-dimensional metric $f(\R)$ theories of gravity are cast into
connection-dynamical formalism with real $\SU(2)$-connections as
configuration variables. Through this formalism, the classical metric
$f(\R)$ theories are quantized by extending the loop quantization
scheme of general relativity. Our results imply that the
non-perturbative quantization procedure of loop quantum gravity is
valid not only for general relativity but also for a rather general
class of 4-dimensional metric theories of gravity.
Distant star clusters of the Milky Way in MOND
Hossein Haghi (IASBS, Zanjan), Holger Baumgardt (Queensland), Pavel
Kroupa (AIfA, Bonn)
http://arxiv.org/abs/1101.1952v1
We determine the mean velocity dispersion of six Galactic outer halo
globular clusters, AM 1, Eridanus, Pal 3, Pal 4, Pal 15, and Arp 2 in
the weak acceleration regime to test classical vs. modified Newtonian
dynamics (MOND). Owing to the non-linearity of MOND's Poisson
equation, beyond tidal effects, the internal dynamics of clusters is
affected by the external field in which they are immersed. For the
studied clusters, particle accelerations are much lower than the
critical acceleration a_0 of MOND, but the motion of stars is neither
dominated by internal accelerations (a_i >> a_e) nor external
accelerations (a_e >> a_i). We use the N-body code N-MODY in our
analysis, which is a particle-mesh-based code with a numerical MOND
potential solver developed by Ciotti, Londrillo, and Nipoti (2006) to
derive the line-of-sight velocity dispersion by adding the external
field effect. We show that Newtonian dynamics predicts a low-velocity
dispersion for each cluster, while in modified Newtonian dynamics the
velocity dispersion is much higher. We calculate the minimum number of
measured stars necessary to distinguish between Newtonian gravity and
MOND with the Kolmogorov-Smirnov test. We also show that for most
clusters it is necessary to measure the velocities of between 30 to 80
stars to distinguish between both cases. Therefore the observational
measurement of the line-of-sight velocity dispersion of these clusters
will provide a test for MOND.
arXiv: 10 January 2010
Amir Hajian, Marco P. Viero, Graeme Addison, Paula Aguirre, John
William Appel, Nick Battaglia, James J. Bock, J. Richard Bond, Sudeep
Das, Mark J. Devlin, Simon R. Dicker, Joanna Dunkley, Rolando Dunner,
Thomas Essinger-Hileman, John P. Hughes, Joseph W. Fowler, Mark
Halpern, Matthew Hasselfield, Matt Hilton, Adam D. Hincks, Renee
Hlozek, Kent D. Irwin, Jeff Klein, Arthur Kosowsky, Yen-Ting Lin,
Tobias A. Marriage, Danica Marsden, Gaelen Marsden, Felipe Menanteau,
Lorenzo Moncelsi, Kavilan Moodley, Calvin B. Netterfield, Michael D.
Niemack, Michael R. Nolta, Lyman A. Page, Lucas Parker, Douglas Scott,
Neelima Sehgal, Jon Sievers, David N. Spergel, Suzanne T. Staggs,
Daniel S. Swetz, Eric R. Switzer, Robert Thornton, Ed Wollack
http://arxiv.org/abs/1101.1517v1
We present measurements of the auto- and cross-frequency correlation
power spectra of the cosmic (sub)millimeter background at: 250, 350,
and 500 um (1200, 860, and 600 GHz) from observations made with the
Balloon-borne Large Aperture Submillimeter Telescope, BLAST; and at
1380 and 2030 um (218 and 148 GHz) from observations made with the
Atacama Cosmology Telescope, ACT. The overlapping observations cover
8.6 deg^2 in an area relatively free of Galactic dust near the south
ecliptic pole (SEP). The ACT bands are sensitive to radiation from the
CMB, the Sunyaev-Zel'dovich (SZ) effect from galaxy clusters, and to
emission by radio and dusty star-forming galaxies (DSFGs), while the
dominant contribution to the BLAST bands is from DSFGs. We confirm and
extend the BLAST analysis of clustering with an independent pipeline,
and also detect correlations between the ACT and BLAST maps at over
25sigma significance, which we interpret as a detection of the DSFGs
in the ACT maps. In addition to a Poisson component in the
cross-frequency power spectra, we detect a clustered signal at
>4sigma, and using a model for the DSFG evolution and number counts,
we successfully fit all our spectra with a linear clustering model and
a bias that depends only on redshift and not on scale. Finally, the
data are compared to, and generally agree with, phenomenological
models for the DSFG population. This study represents a first of its
kind, and demonstrates the constraining power of the cross-frequency
correlation technique to constrain models for the DSFGs. Similar
analyses with more data will impose tight constraints on future
models.
Primordial non-Gaussianities from inflation
Hael Collins (The Niels Bohr International Academy)
http://arxiv.org/abs/1101.1308v1
These notes present a detailed introduction to Maldacena's
calculation of the cubic terms in the inflationary action. These
interactions are important since they produce the most readily
observable evidence for a non-Gaussian component in the pattern of
primordial fluctuations produced by inflation. In the simplest class
of inflationary theories, those with only a single scalar field
participating in the inflationary era, these non-Gaussianities are
predicted to be extremely small, as will be reviewed here.
Galilean-invariant scalar fields can strengthen gravitational lensing
Mark Wyman
http://arxiv.org/abs/1101.1295v1
The mystery of dark energy suggests that there is new gravitational
physics at low energies and on long length scales. On the other hand,
low mass degrees of freedom in gravity are strictly limited by
observations within the solar system. A compelling way to resolve this
apparent contradiction is to add a galilean-invariant scalar field to
gravity. Called galileons, these scalars have strong self interactions
near overdensities, like the solar system, that suppress their effects
on the motion of massive particles. These non-linearities are weak on
cosmological scales, permitting new physics to operate. In this note,
we point out that extending galilean invariance to the coupling of
galileons to stress-energy -- as was first done in the case of massive
gravity -- can have a surprising phenomenological consequence:
enhanced gravitational lensing. Weak lensing observations should be
able to detect or rule out this effect.
Sunday, January 9, 2011
arXiv: 7 January 2011
Discovery and Cosmological Implications of SPT-CL J2106-5844, the Most Massive Known Cluster at z > 1
Sub-millimetre galaxies reside in dark matter halos with masses greater than 3x10^11 solar masses
General Covariance in Gravity at a Lifshitz Point
arXiv: 6 January 2011
Gravitational microlensing in modified gravity theories: Inverse-square theorem
http://arxiv.org/abs/1101.0864v1
Cosmological structure formation with clustering quintessence
Saturday, January 8, 2011
arXiv: 5 January 2010
Future Oscillations around Phantom Divide in f(R) Gravity
f(R) Gravity and its Cosmological Implications
http://arxiv.org/abs/1101.0716v1
Tuesday, January 4, 2011
arXiv: 4 January 2011
The Sunyaev-Zel'dovich Array: Constraining a new pressure profile for fitting SZE observations of galaxy clusters
The SZA 30-GHz receiver system probes angular scales ~1-5'. A model that can accurately describe a cluster's pressure profile over a correspondingly broad range of radii is therefore required. In the analysis presented here, I fit a 2-parameter, radial pressure profile, derived from simulations and detailed X- ray analysis of relaxed clusters, to SZA observations of three clusters with exceptionally high quality X-ray data. From the joint analysis of the SZE and X-ray data, I derive physical properties of the cluster, such as gas and total mass, gas fraction and the integrated Compton y -parameter.
The parameters derived from the joint fit to SZE+X-ray data agree well with a detailed, independent, X-ray-only analysis of these same clusters. When combined with X-ray imaging data, this new pressure profile yields an independent estimate of the electron temperature profile that is in good agreement with spectroscopic X-ray determinations. In addition to yielding relationships between cluster observables and physical cluster properties, this model could prove to be a useful tool in helping to constrain the temperatures of high redshift clusters, for which X-ray spectroscopic data are difficult to obtain.