Munch June 26th, 2006

                               


 


 

 

 

 

 

 

 

 

 

 

 

 

 

 

 


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Nature Article




Constraining Primordial Non-Gaussianities from the WMAP2 2-1 Cumulant Correlator Power Spectrum

Authors: Gang Chen, Istvan Szapudi
Comments: 4 pages,2 figures; typos corrected, references changed
We measure the 2-1 cumulant correlator power spectrum $C^{21}_l$, a degenerate bispectrum, from the second data release of the Wilkinson Microwave Anisotropy Probe (WMAP). Our high resolution measurements with SpICE span a large configuration space ($\simeq 168\times999$) corresponding to the possible cross-correlations of the maps recorded by the different differencing assemblies. We present a novel method to recover the eigenmodes of the correspondingly large Monte Carlo covariance matrix. We examine its eigenvalue spectrum and use random matrix theory to show that the off diagonal terms are dominated by noise. We minimize the $\chi^2$ to obtain constraints for the non-linear coupling parameter $f_{NL} = 22 \pm 52 (1\sigma)$.

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Estimators for local non-Gaussianities

Authors: Paolo Creminelli (ICTP, Trieste), Leonardo Senatore (MIT), Matias Zaldarriaga (Harvard-Smithsonian Ctr. Astrophys. & Harvard U., Phys. Dept.)
Comments: 25 pages
Report-no: HUTP-06/A0016, MIT-CTP 3737, IC/2006/028
We study the Likelihood function of data given f_NL for the so-called local type of non-Gaussianity. In this case the curvature perturbation is a non-linear function, local in real space, of a Gaussian random field. We compute the Cramer-Rao bound for f_NL and show that for small values of f_NL the 3-point function estimator saturates the bound and is equivalent to calculating the full Likelihood of the data. However, for sufficiently large f_NL, the naive 3-point function estimator has a much larger variance than previously thought. In the limit in which the departure from Gaussianity is detected with high confidence, error bars on f_NL only decrease as 1/ln Npix rather than Npix^-1/2 as the size of the data set increases. We identify the physical origin of this behavior and explain why it only affects the local type of non-Gaussianity, where the contribution of the first multipoles is always relevant. We find a simple improvement to the 3-point function estimator that makes the square root of its variance decrease as Npix^-1/2 even for large f_NL, asymptotically approaching the Cramer-Rao bound. We show that using the modified estimator is practically equivalent to computing the full Likelihood of f_NL given the data. Thus other statistics of the data, such as the 4-point function and Minkowski functionals, contain no additional information on f_NL. In particular, we explicitly show that the recent claims about the relevance of the 4-point function are not correct. By direct inspection of the Likelihood, we show that the data do not contain enough information for any statistic to be able to constrain higher order terms in the relation between the Gaussian field and the curvature perturbation, unless these are orders of magnitude larger than the size suggested by the current limits on f_NL.

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Transients from Initial Conditions in Cosmological Simulations

Authors: M. Crocce, S. Pueblas, R. Scoccimarro
Comments: 14 pages, 14 figures, code to generate 2LPT initial conditions available at this http URL
We study the impact of setting initial conditions in numerical simulations using the standard procedure based on the Zel'dovich approximation (ZA). As it is well known from perturbation theory, ZA initial conditions have incorrect second and higher-order growth and therefore excite long-lived transients in the evolution of the statistical properties of density and velocity fields. We also study the improvement brought by using more accurate initial conditions based on second-order Lagrangian perturbation theory (2LPT). We show that 2LPT initial conditions reduce transients significantly and thus are much more appropriate for numerical simulations devoted to precision cosmology. Using controlled numerical experiments with ZA and 2LPT initial conditions we show that simulations started at redshift z_i=49 using the ZA underestimate the power spectrum in the nonlinear regime by about 2,4,8 % at z=0,1,3 respectively, whereas the mass function of dark matter halos is underestimated by 5% at m=10^15 M_sun/h (z=0) and 10% at m=2x10^14M_sun/h (z=1). The clustering of halos is also affected to the few percent level at z=0. These systematics effects are typically larger than statistical uncertainties in recent mass function and power spectrum fitting formulae extracted from numerical simulations. At large scales, the measured transients in higher-order correlations can be understood from first principle calculations based on perturbation theory.

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Cosmological Constraints from the Red-Sequence Cluster Survey

Authors: Michael D. Gladders, H.K.C. Yee, Subhabrata Majumdar, L. Felipe Barrientos, Henk Hoekstra, Patrick B. Hall, Leopoldo Infante
Comments: 18 pages, 4 figures, 3 tables
[abridged] We present a first cosmological analysis of a refined cluster catalog from the Red-Sequence Cluster Survey (RCS). The input cluster sample is derived from 72.07 square degrees of imaging data [...] The catalog contains 956 clusters over 0.35<z<0.95, limited by cluster richness and richness error. The calibration of the survey images has been extensively cross-checked against publicly available Sloan Digital Sky Survey imaging [...] We analyze the cluster sample via a general self-calibration technique including scatter in the mass-richness relation [...]. We fit simultaneously for Omega_M and sigma_8, and four parameters describing the calibration of cluster richness to mass, its evolution with redshift, and scatter in the richness-mass relation. The principal goal of this general analysis is to establish the consistency (or lack thereof) between the fitted parameters (both cosmological and cluster mass observables) and available results on both from independent measures. From an unconstrained analysis, Omega_M and sigma_8 are 0.31+0.11-0.10 and 0.67+0.18-0.13 respectively. An analysis including Gaussian priors on the slope and zeropoint of the mass-richness relation gives very similar results: 0.30+0.12-0.11 and 0.70+0.27-0.15. Both analyses are in good agreement with the current literature. The parameters describing the mass-richness relation in the unconstrained fit are also eminently reasonable and agree with existing follow-up data on both the RCS-1 and other cluster samples. Our results directly demonstrate that future surveys (optical and otherwise), with much larger samples of clusters, can give constraints competitive with other probes of cosmology.

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The Virial Mass Function of Nearby SDSS Galaxy Clusters

Authors: Kenneth Rines (Yale/YCAA), Antonaldo Diaferio (Torino), Priyamvada Natarajan (Yale/YCAA)
Comments: 22 pages, 11 figures, submitted to ApJ
We present a new determination of the cluster mass function and velocity dispersion function in a volume $\sim10^7 h^3$Mpc$^{-3}$ using the Fourth Data Release of the Sloan Digital Sky Survey (SDSS). We use the caustic technique to remove foreground and background galaxies. The cluster virial mass function agrees very well with recent estimates from both X-ray observations and cluster richnesses. The mass function lies between those predicted by the First-Year and Three-Year WMAP data. We constrain the cosmological parameters $\Omega_m$ and $\sigma_8$ and find good agreement with WMAP and constraints from other techniques. With the CIRS mass function alone, we estimate $\Omega_m=0.23^{+0.14}_{-0.09}$ and $\sigma_8=0.91^{+0.17}_{-0.19}$, or $\sigma_8=0.81\pm$0.03 when holding $\Omega_m=0.3$ fixed. We also use the WMAP parameters as priors and constrain velocity segregation in clusters. Using the First and Third-Year results, we infer velocity segregation of $\sigma_{gxy}/\sigma_{DM}\approx0.91\pm$0.04 or 1.30$\pm$0.05 respectively. We compare the velocity dispersion function of clusters to that of early-type galaxies and conclude that clusters comprise the high-velocity end of the velocity dispersion function of dark matter haloes. The evolution of cluster abundances provides constraints on dark energy models; the mass function presented here offers an important low redshift calibration benchmark.

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Inflation and WMAP three year data: Features have a Future!

Authors: Laura Covi, Jan Hamann, Alessandro Melchiorri, Anze Slosar, Irene Sorbera
Comments: 7 pages, 11 figures
Report-no: DESY 06-089
The new three year WMAP data seem to confirm the presence of non-standard large scale features in the Cosmic Microwave Anisotropies power spectrum. While these features may hint at uncorrected experimental systematics, it is also possible to generate, in a cosmological way, oscillations on large angular scales by introducing a sharp step in the inflaton potential. Using current cosmological data, we derive constraints on the position, magnitude and gradient of a possible step in the inflaton potential. We show that a step in the potential, while strongly constrained by current data, is still allowed and may provide an interesting explanation to the currently measured deviations from the standard featureless spectrum.

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Difficulties for Compact Composite Object Dark Matter

Authors: Daniel T. Cumberbatch, Joseph Silk, Glenn D. Starkman
Recently Zhitnitsky suggested ``that DM particles are strongly interacting composite macroscopically large objects ... made of well known light quarks (or >... antiquarks)." In doing so he argued that these compact composite objects (CCOs) are ``natural explanations of many observed data, such as [the] 511 keV line from the bulge of our galaxy" and the CHANDRA-observed excess of diffuse X-ray emission toward the galactic center. Here we argue that the annihilation of interstellar electrons (or positrons) off positrons (or electrons) in the the CCO does not lead to the observed narrow 511 keV line, but to a broad continuum due to the high densities of the CCO-confined leptons. We argue further that in order to generate the observed flux of X-rays, the CCOs in the galactic centre would only require a temperature of 1 eV, and therefore unlikely to be the dominant heat source for the surrounding 8 keV plasma. While these observations do not rule out CCOs as galactic dark matter, they do weaken the motivation for them.

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The Price of WMAP Inflation in Supergravity

Authors: J. Ellis, Z. Lalak, S. Pokorski, K. Turzynski
Comments: 15 pages, 6 figures, plain Latex
Report-no: CERN-PH-TH/2006-099
The three-year data from WMAP are in stunning agreement with the simplest possible quadratic potential for chaotic inflation, as well as with new or symmetry-breaking inflation. We investigate the possibilities for incorporating these potentials within supergravity, particularly of the no-scale type that is motivated by string theory. Models with inflation driven by the matter sector may be constructed in no-scale supergravity, if the moduli are assumed to be stabilised by some higher-scale dynamics and at the expense of some fine-tuning. We discuss specific scenarios for stabilising the moduli via either D- or F-terms in the effective potential, and survey possible inflationary models in the presence of D-term stabilisation.

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