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Elena Pierpaoli

Publications and source records attributed to Elena Pierpaoli.

69 records · Page 4Linked to original sources

Massive galaxy clusters and the origin of Ultra High Energy Cosmic Rays

We investigate whether ultra--high energy cosmic rays (UHECR) may be preferentially produced in massive galaxy clusters, by looking for correlations between UHECR directions and those of x-ray clusters. We find an excess-above-random of high energy cosmic rays which correlate with massive galaxy cluster positions. For cosmic rays with energies above 50 EeV the observed correlation is the strongest or angles of 1.2-1.6 degrees where it has a chance probability of about 0.1%. Including lower energy cosmic rays in the sample causes the angle where the most significant correlation is found to increase, as would be expected by virtue of instrumental and magnetic smearing increasing at lower energy. These results suggest that some UHECR are produced in galaxy clusters, or in objects that preferentially populate galaxy clusters.

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Probing the largest scale structure in the universe with polarization map of galaxy clusters

We introduce a new formalism to describe the polarization signal of galaxy clusters on the whole sky. We show that a sparsely sampled, half-sky map of the cluster polarization signal at $z\sim 1$ would allow to better characterize the very large scale density fluctuations. While the horizon length is smaller in the past, two other competing effects significantly remove the contribution of the small scale fluctuations from the quadrupole polarization pattern at $z\sim 1$. For the standard Lambda-CDM universe with vanishing tensor mode, the quadrupole moment of the temperature anisotropy probed by WMAP is expected to have a ~32% contribution from fluctuations on scales below 6.3h^{-1}Gpc. This percentage would be reduced to ~2% level for the quadrupole moment of polarization pattern at $z\sim 1$. A cluster polarization map at $z \sim 1$ would shed light on the potentially anomalous features of the largest scale structure in the observable universe.

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Finding SZ clusters in the ACBAR maps

We present a new method for component separation from multifrequency maps aimed to extract Sunyaev-Zeldovich (SZ) galaxy clusters from Cosmic Microwave Background (CMB) experiments. This method is best suited to recover non--Gaussian, spatially localized and sparse signals. We apply our method on simulated maps of the ACBAR experiment. We find that this method improves the reconstruction of the integrated $y$ parameter by a factor three with respect to the Wiener filter case. Moreover, the scatter associated with the reconstruction is reduced by 30 per cent.

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Accretion flows in early-type galaxies and CMB experiments

We investigate the possible contribution from the emission of accretion flows around supermassive black holes in early type galaxies to current measurements of the Cosmic Microwave Background (CMB) at radio frequencies. We consider a range of luminosities suggested by targeted radio observations and accretion models and compute the residual contribution of these sources to the spectrum and bispectrum of the observed CMB maps. As for high-resolution CMB experiments, we find that the unresolved component of these sources could make up to ~40-50% of the observed CBI and BIMA power spectrum at l > 2000. As a consequence, the inferred sigma_8^{SZ} value could be biased high by up to 6-7%. As for all sky experiments, we find that the contribution of accretion-flow sources to the WMAP bispectrum is at the 2-3 per cent level at most. At the flux limit that Planck will achieve, however, these sources may contribute up to 15 per cent of the bispectrum in the 60-100 GHz frequency range. Moreover, Planck should detect hundreds of these sources in the 30-300 GHz frequency window. These detections, possibly coupled with galaxy type confirmation from optical surveys, will allow number counts to put tighter constraints on early-type galaxies radio luminosity and accretion flows properties. These sources may also contribute up to the 30 per cent level to the residual radio sources power spectrum in future high-resolution SZ surveys (like ACT or APEX) reaching mJy flux limits.

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Decaying particles and the reionization history of the Universe

We investigate the possibility that the Universe is reionized by the decay products of heavy particles. In particular we study under which circumstances this decay may produce a significant reionization at high redshift ($z \simeq 20$), as requested by the WMAP result.Extra sources of reionization at high redshifts increase the recombination rate. As a result, the number density of decaying particles required to produce a high level of ionization at $z \simeq 10-20$ is significantly higher ($\simeq 300$ times) than previously estimated. Moreover, the ionization produced by decay particles implies a high optical depth even if the maximum level of ionization ever produced is of the order of $10^{-2}$. In order to match the cosmic microwave background polarization power spectrum, other significant sources of reionization are needed at low redshift. Decaying particles producing a ionization fraction $x \simeq 0.5$ at $z \simeq 20$ would imply an optical depth much too high to fit the cosmic microwave background spectra at $l \ge 30$. For decay times $t_{dec} < 2 \times 10^{16} {\rm s}$, recent cosmic microwave background and large scale structure data limits the primordial abundance of the decaying particles to $Ω_x \le 21 \times 10^{-9} (1+z)^3$ at 95 % C.L., and favors long decay times. The data do not favor this reionization model versus the instantaneous reionization one. We also find that the decay of these heavy particles significantly heats up the medium, bringing the expected $y$ distortion to unobservable levels.

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Measurement of the Sunyaev-Zel'dovich Increment in Massive Galaxy Clusters

We have detected the Sunyaev-Zel'dovich (SZ) increment at 850 microns in two galaxy clusters (Cl 0016+16 and MS 1054.4-0321) using SCUBA (Sub-millimetre Common User Bolometer Array) on the James Clerk Maxwell Telescope. Fits to the isothermal βmodel yield a central Compton y parameter of (2.2 \pm 0.7) x 10^{-4} and a central 850 micron flux of ΔI_{0} = 2.2 \pm 0.7 mJy/beam in Cl 0016. This can be combined with decrement measurements to infer y = (2.38 \pm_{0.34}^{0.36}) x 10^{-4} and v_{pec} = 400 \pm_{1400}^{1900} km/s. In MS 1054 we find a peak 850 micron flux of ΔI_{0} = 2.0 \pm 1.0 mJy/beam and y = (2.0 \pm 1.0) x 10^{-4}. To be successful such measurements require large chop throws and non-standard data analysis techniques. In particular, the 450 micron data are used to remove atmospheric variations in the 850 micron data. An explicit annular model is fit to the SCUBA difference data in order to extract the radial profile, and separately fit to the model differences to minimize the effect of correlations induced by our scanning strategy. We have demonstrated that with sufficient care, SCUBA can be used to measure the SZ increment in massive, compact galaxy clusters.

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Constraints on the cosmic neutrino background

The radiative component of the Universe has a characteristic impact on both large scale structure (LSS) and the cosmic microwave background radiation (CMB). We use the recent WMAP data, together with previous CBI data and 2dF matter power spectrum, to constrain the effective number of neutrino species $N_{eff}$ in a general Cosmology. We find that $N_{eff}=4.31$ with a 95 per cent C.L. $1.6 \le N_{eff} \le 7.1$. If we include the $H_0$ prior from the HST project we find the best fit $N_{eff}=4.08$ and $1.90 \le N_{eff} \le 6.62$ for 95 per cent C.L. The curvature we derive is still consistent with flat, but assuming a flat Universe from the beginning implies a bias toward lower $N_{eff}$, as well as artificially smaller error bars. Adding the Supernovae constraint doesn't improve the result. We analyze and discuss the degeneracies with other parameters, and point out that probes of the matter power spectrum on smaller scales, accurate independent $σ_8$ measurements, together with better independent measurement of $H_0$ would help in breaking the degeneracies.

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Point sources in the MAP sky maps

We discuss point sources foregrounds for the MAP experiment. We consider several possible strategies for removing them and we assess how the statistics of the CMB signal are affected by the residual sources. Assuming a power law distribution for the point sources, we propose a method aimed to determine the slope of the distribution from the analysis of the moments of the observed maps. The same method allows for a determination of the underlying CMB variance. We conclude that the best strategy for point sources finding is the simultaneous thresholding of the filtered map at all frequencies, with a relatively low threshold. With this strategy, we expect to find 70 (95)% of the sources above 3 (4) $σ$. Assuming the most conservative case for point sources detection, the recovered slope of the point sources distribution is $2.55 \pm 0.15$, for a fiducial $n=2.5$ value. The recovered CMB pus noise map variance is within 0.2% from the real one, with a standard deviation of $0.31 %$, while Cosmic variance contributes 2.2% to the same CMB plus noise map.

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Cosmological Difficulties with Modified Newtonian Dynamics (or: La Fin du MOND?)

The cold dark matter paradigm has been extremely successful for explaining a wide range of cosmological phenomena. Nevertheless, since evidence for non-baryonic dark matter remains indirect, all reasonable alternatives should be explored. One proposed idea, involving a fundamental acceleration scale a_0 = 1-2e-10 m/s^2, is called MOdified Newtonian Dynamics or MOND. MOND was suggested to explain the flat rotation curves of galaxies without the need for dark matter. Whether or not it can adequately fit the available data has been debated for almost 20 years (and we summarise many of these studies), but only recently have there been attempts to extend MOND to larger scale regimes. We discuss how the basic properties of MOND make it at best ambiguous to apply these ideas to cosmological scales. We emphasize the difficulties inherent in developing a full theory in which to embed MOND. Without such a theory there is no obviously consistent way to discuss the early Universe and the growth of perturbations. Recent claims that MONDian cosmology works very well are therefore not supportable. We also provide an argument for why a_0~cH_0 naturally, a coincidence which is often suggested as a motivation for taking MOND seriously. We discuss other alternative theories of gravity concluding, as others have, that no metric theory extensions appear workable for explaining rotation curves as well as other observed phenomena. The whole premise of many of these attempts is fatally flawed - galaxies are not pre-selected, discrete, isolated regions which formed monolithically and around which one can construct an axially-symmetric dynamical model in order to remove the need for dark matter. In the modern view, galaxies are part of a dynamic continuum of objects which collectively make up the evolving large-scale structure of the universe.

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Boomerang returns unexpectedly

Experimental study of the anisotropy in the cosmic microwave background (CMB) is gathering momentum. The eagerly awaited Boomerang results have lived up to expectations. They provide convincing evidence in favor of the standard paradigm: the Universe is close to flat and with primordial fluctuations which are redolent of inflation. Further scrutiny reveals something even more exciting however -- two hints that there may be some unforeseen physical effects. Firstly the primary acoustic peak appears at slightly larger scales than expected. Although this may be explicable through a combination of mundane effects, we suggest it is also prudent to consider the possibility that the Universe might be marginally closed. The other hint is provided by a second peak which appears less prominent than expected. This may indicate one of a number of possibilities, including increased damping length or tilted initial conditions, but also breaking of coherence or features in the initial power spectrum. Further data should test whether the current concordance model needs only to be tweaked, or to be enhanced in some fundamental way.

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Still flat after all these years

The Universe could be spatially flat, positively curved or negatively curved. Each option has been popular at various times, partly affected by an understanding that models tend to evolve away from flatness. The curvature of the Universe is amenable to measurement, through tests such as the determination of the angles of sufficiently large triangles. The angle subtended by the characteristic scale on the Cosmic Microwave sky provides a direct test, which has now been realised through a combination of exquisite results from a number of CMB experiments. After a long and detailed investigation, with many false clues, it seems that the mystery of the curvature of the Universe is now solved. It's an open and shut case: the Universe is flat.

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A Characteristic Scale on the Cosmic Microwave Sky

The current suite of results from Cosmic Microwave Background anisotropy experiments is fulfilling the promise of providing extraordinary levels of discrimination between cosmological models. We calculate a binned anisotropy power spectrum, which we tabulate, along with error bars and bin-to-bin correlations, so that it can be easily used for constraining models. The resulting power spectrum is flat at large angles, with a gradual rise to a prominent peak at around 0.5 degrees and a decrease thereafter. This is precisely the shape predicted by inflationary-inspired adiabatic models. Within that class of cosmologies, this characteristic scale imprinted on the CMB sky can be used to infer that the geometry of the Universe is very close to flat. The next wave of CMB results should add fuel to the debate about whether or not the Universe once inflated, as well as beginning in earnest the task of measuring cosmological parameters.

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Microwave background anisotropies and large scale structure constraints on isocurvature modes in a two-field model of inflation

In this paper we study the isocurvature mode contribution to the cosmic microwave background anisotropies and the large scale structure power spectrum, for a two-field model of inflation proposed by Linde and Mukhanov. We provide constraints on the parameters of the model by comparing its predictions with observations of the microwave background anisotropies, large scale structure data on the galaxy power spectrum, and the number density of nearby galaxy clusters. We find that such models are consistent with observations for a narrow range of parameters. As our main result, we find that only a very small isocurvature component is allowed, $\al \le 0.006$, for any underlying Friedmann model. Furthermore, we give the expected resolution with which the model parameters will be determined from future satellite missions like MAP and Planck, for a fiducial flat $Λ$CDM model. We find that Planck mission will be able to detect such small contributions, especially if polarization information is included. The isocurvature spectral index $\niso$ will also be determined with better than 8% precision.

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The Formation of Cosmic Structures in a Light Gravitino Dominated Universe

We analyse the formation of cosmic structures in models where the dark matter is dominated by light gravitinos with mass of $ 100$ eV -- 1 keV, as predicted by gauge-mediated supersymmetry (SUSY) breaking models. After evaluating the number of degrees of freedom at the gravitinos decoupling ($g_*$), we compute the transfer function for matter fluctuations and show that gravitinos behave like warm dark matter (WDM) with free-streaming scale comparable to the galaxy mass scale. We consider different low-density variants of the WDM model, both with and without cosmological constant, and compare the predictions on the abundances of neutral hydrogen within high-redshift damped Ly--$α$ systems and on the number density of local galaxy clusters with the corresponding observational constraints. We find that none of the models satisfies both constraints at the same time, unless a rather small $Ω_0$ value ($\mincir 0.4$) and a rather large Hubble parameter ($\magcir 0.9$) is assumed. Furthermore, in a model with warm + hot dark matter, with hot component provided by massive neutrinos, the strong suppression of fluctuation on scales of $\sim 1\hm$ precludes the formation of high-redshift objects, when the low--$z$ cluster abundance is required. We conclude that all different variants of a light gravitino DM dominated model show strong difficulties for what concerns cosmic structure formation. This gives a severe cosmological constraint on the gauge-mediated SUSY breaking scheme.

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Large-Scale Structure in Mixed Dark Matter Models with a Non-thermal Volatile Component

We investigate the properties of large--scale structure predicted in a class of mixed dark matter models in which the volatile component (made of particles with high rms velocity) derives from the decay of a heavier particle. Such models based on cold+volatile dark matter (CVDM) differ from the standard mixture of CDM and massive neutrinos, usually known as CHDM, in that they involve a component which has a non--thermal phase space distribution function. As a consequence, and differently from CHDM models, the value of the redshift at which volatile particles become non relativistic, $z_{nr}$, can be varied almost independently of the volatile fraction, $Ω_X$. We compute transfer functions for a selection of such models, having $0.1\le Ω_X\le 0.5$ and different values of $z_{nr}$. Using linear theory and assuming a scale--free primordial spectrum, we compare such models with observational constraints on large--scale galaxy clustering and bulk flows, as well as on the abundance of galaxy clusters and high--redshift damped Ly$α$ systems. We find that these constraints enable us to discriminate between different $Ω_X$ and $z_{nr}$; within the range of the models inspected, those which can be most easily accommodated by the data correspond to the parameter choice $Ω_X\simeq 0.2$ and $z_{nr} \simeq 2\times 10^4Ω_X$.

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