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      Hierarchy of N-point functions in the LCDM and ReBEL cosmologies

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          Abstract

          In this work we investigate higher order statistics for the \(\lcdm\) and ReBEL scalar-interacting dark matter models by analyzing \(180\hmpc\) dark matter N-body simulation ensembles. The N-point correlation functions and the related hierarchical amplitudes, such as skewness and kurtosis, are computed using the Count-In-Cells method. Our studies demonstrate that the hierarchical amplitudes \(S_n\) of the scalar-interacting dark matter model significantly deviate from the values in the \(\lcdm\) cosmology on scales comparable and smaller then the screening length \(r_s\) of a given scalar-interacting model. The corresponding additional forces that enhance the total attractive force exerted on dark matter particles at galaxy scales lowers the values of the hierarchical amplitudes \(S_n\). We conclude that hypothetical additional exotic interactions in the dark matter sector should leave detectable markers in the higher-order correlation statistics of the density field. We focussed in detail on the redshift evolution of the dark matter field's skewness and kurtosis. From this investigation we find that the deviations from the canonical \(\lcdm\) model introduced by the presence of the ``fifth'' force attain a maximum value at redshifts \(0.5<z<2\). We therefore conclude that moderate redshift data are better suited for setting observational constraints on the investigated ReBEL models.

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          Measurements of Omega and Lambda from 42 High-Redshift Supernovae

          We report measurements of the mass density, Omega_M, and cosmological-constant energy density, Omega_Lambda, of the universe based on the analysis of 42 Type Ia supernovae discovered by the Supernova Cosmology Project. The magnitude-redshift data for these SNe, at redshifts between 0.18 and 0.83, are fit jointly with a set of SNe from the Calan/Tololo Supernova Survey, at redshifts below 0.1, to yield values for the cosmological parameters. All SN peak magnitudes are standardized using a SN Ia lightcurve width-luminosity relation. The measurement yields a joint probability distribution of the cosmological parameters that is approximated by the relation 0.8 Omega_M - 0.6 Omega_Lambda ~= -0.2 +/- 0.1 in the region of interest (Omega_M 0) = 99%, including the identified systematic uncertainties. The best-fit age of the universe relative to the Hubble time is t_0 = 14.9{+1.4,-1.1} (0.63/h) Gyr for a flat cosmology. The size of our sample allows us to perform a variety of statistical tests to check for possible systematic errors and biases. We find no significant differences in either the host reddening distribution or Malmquist bias between the low-redshift Calan/Tololo sample and our high-redshift sample. The conclusions are robust whether or not a width-luminosity relation is used to standardize the SN peak magnitudes.
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            Nearby galaxies as pointers to a better theory of cosmic evolution.

            The great advances in the network of cosmological tests show that the relativistic Big Bang theory is a good description of our expanding Universe. However, the properties of nearby galaxies that can be observed in greatest detail suggest that a better theory would describe a mechanism by which matter is more rapidly gathered into galaxies and groups of galaxies. This more rapid growth occurs in some theoretical ideas now under discussion.
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              A comparison of cosmological models using recent supernova data

              We study the expansion history of the universe up to a redshift of z=1.75 using the 194 recently published SnIa data by Tonry et. al. and Barris et. al. In particular we find the best fit forms of several cosmological models and \(H(z)\) ansatze, determine the best fit values of their parameters and rank them according to increasing value of \(\chi_{min}^2\) (the minimum value of \(\chi^2\) for each \(H(z)\) ansatz). We use a prior of \(\Omega_{0m} = 0.3\) and assume flat geometry of the universe. No prior assumptions are made about validity of energy conditions. The fitted models are fourteen and include SCDM, LCDM, dark energy with constant equation of state parameter \(w\) (quiessence), third order polynomial for \(H(1+z)\), Chaplygin gas, Cardassian model, \(w(z)=w_0 + w_1 z\), \(w(z)=w_0 + z w_1/(1+z)\), an oscillating ansatz for \(H(z)\) etc. All these models with the exception of SCDM are consistent with the present data. However, the quality of the fit differs significantly among them and so do the predicted forms of \(w(z)\) and \(H(z)\) at best fit. The worst fit among the data-consistent models considered corresponds to the simplest model LCDM (\(\chi_{min}^2 = 198.7\) for \(\Omega_{0m} = 0.34\)) while the best fit is achieved by the three parameter oscillating ansatz (\(\chi_{min}^2 = 194.1\)). Most of the best fit ansatze have an equation of state parameter \(w(z)\) that varies between \(w(z) \simeq -1\) for \(z 0\) for \(z>1\). This implies that the sign of the pressure of the dark energy may be alternating as the redshift increases. The goodness of fit of the oscillating \(H(z)\) ansatz lends further support to this possibility.
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                Author and article information

                Journal
                23 August 2010
                2010-10-29
                Article
                10.1103/PhysRevD.82.103536
                1008.3930
                572672ef-ffe5-44f1-bd63-f2720136ad5a

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                20 pages, 13 figures, accepted for publication in Phys. Rev. D, minor review, 1 new figure added, most of the figures replaced, main conclusions unchanged
                astro-ph.CO hep-ph

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