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Journal ArticleDOI

Relativistic Effects of our Galaxy's Motion on Circles-in-the-sky

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TLDR
In this paper, the geometric effects of our galaxy's peculiar motion on the circles-in-the-sky were studied and an explicit expression for the radius and center position of such an observed circle in the sky, as well as the angular displacement of points on the circle, were derived.
Abstract
We study the geometric effects of our galaxy's peculiar motion on the circles-in-the-sky. We show that the shape of these circles-in-the-sky remains circular, as detected by a local observer with arbitrary peculiar velocity. Explicit expressions for the radius and center position of such an observed circle-in-the-sky, as well as for the angular displacement of points on the circle, are derived. In general, a circle is detected as a circle of different radius, displaced relative to its original position, and centered at a point which does not correspond to its detected center in the comoving frame. Further, there is an angular displacement of points on the circles. These effects all arise from aberration of cosmic microwave background radiation, exhausting the purely geometric effects due to the peculiar motion of our galaxy, and are independent of both the large scale curvature of space and the expansion of the universe, since aberration is a purely local phenomenon. For a Lorentz-boosted observer with the speed of our entire galaxy, the maximum (detectable) changes in the angular radius of a circle, its maximum center displacement, as well as the maximum angular distortion are shown all to be of order $\beta=(v/c)$ radians. In particular, two back-to-back matching circles in a finite universe will have an upper bound of $2|\beta|$ in the variation of either their radii, the angular position of their centers, or the angular distribution of points.

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Journal ArticleDOI

Dipoles in the sky

TL;DR: In this article, the amplitude and direction of dipolar modulations in the number count of sources projected along the line of sight are constrained using data from large-scale-structure surveys spanning a wide range of wavelengths.
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Cmb multipole measurements in the presence of foregrounds

TL;DR: In this paper, a minimum-variance method for computing the power spectrum of the cosmic microwave background spherical harmonic coefficients was proposed. But the method is not suitable for the case of incomplete sky coverage and foreground contamination.
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Distinguishing between void models and dark energy with cosmic parallax and redshift drift

TL;DR: In this paper, the authors show that the degeneracy between Lemaitre-Tolman-Bondi void models and more traditional dark-energy theories can be broken with high confidence levels in the course of a decade.
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Generalized Chaplygin gas model, supernovae, and cosmic topology

TL;DR: In this article, the authors examined the effect of knowledge of spatial topology on the parameters of the generalized Chaplygin gas (GCG) model for unification of dark energy and dark matter.
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Measuring our peculiar velocity by ``pre-deboosting'' the CMB

TL;DR: In this article, it was shown that our peculiar velocity β with respect to the CMB induces mixing among multipoles and off-diagonal correlations at all scales which can be used as a measurement of β, which is independent of the standard measurement using the temperature dipole.
References
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First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Preliminary Maps and Basic Results

Abstract: We present full sky microwave maps in five bands (23 to 94 GHz) from the WMAP first year sky survey. Calibration errors are 1 per mode to l=658. The temperature-polarization cross-power spectrum reveals both acoustic features and a large angle correlation from reionization. The optical depth of reionization is 0.17 +/- 0.04, which implies a reionization epoch of 180+220-80 Myr (95% CL) after the Big Bang at a redshift of 20+10-9 (95% CL) for a range of ionization scenarios. This early reionization is incompatible with the presence of a significant warm dark matter density. The age of the best-fit universe is 13.7 +/- 0.2 Gyr old. Decoupling was 379+8-7 kyr after the Big Bang at a redshift of 1089 +/- 1. The thickness of the decoupling surface was dz=195 +/- 2. The matter density is Omega_m h^2 = 0.135 +0.008 -0.009, the baryon density is Omega_b h^2 = 0.0224 +/- 0.0009, and the total mass-energy of the universe is Omega_tot = 1.02 +/- 0.02. The spectral index of scalar fluctuations is fit as n_s = 0.93 +/- 0.03 at wavenumber k_0 = 0.05 Mpc^-1, with a running index slope of dn_s/d ln k = -0.031 +0.016 -0.018 in the best-fit model. This flat universe model is composed of 4.4% baryons, 22% dark matter and 73% dark energy. The dark energy equation of state is limited to w<-0.78 (95% CL). Inflation theory is supported with n_s~1, Omega_tot~1, Gaussian random phases of the CMB anisotropy, and superhorizon fluctuations. An admixture of isocurvature modes does not improve the fit. The tensor-to-scalar ratio is r(k_0=0.002 Mpc^-1)<0.90 (95% CL).
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Asymmetries in the CMB anisotropy field

TL;DR: In this paper, two independent but complementary statistical analyses of the WMAP first-year data, based on the power spectrum and N-point correlation functions, are presented. But the results are stable with respect to the choice of Galactic cut and also with respect with the frequency band.
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