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Nearby Supernova Factory: Étalonnage des données de SNIFS et ...

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tel-00372504, version 1 - 1 Apr 2009<br />

CHAPTER 2. OBSERVATIONAL COSMOLOGY<br />

By analyzing the anisotropies map (Fig. 2.1a), one can extract the fundamental oscillatory<br />

mo<strong>de</strong> and corresponding harmonics, and obtain its power spectrum (Fig. 2.1b). The exact form<br />

of the peaks of the power spectrum <strong>de</strong>pends on the matter content of the universe, thus the<br />

measurement of its shape (a standard ruler), yields precise information about many cosmological<br />

param<strong>et</strong>ers. These measurements, while not probing dark energy directly, provi<strong>de</strong> constraints<br />

like the flatness (Ωk), or the baryon (Ωb) and dark matter <strong>de</strong>nsities (Ωc), that can be used to<br />

infer ΩΛ.<br />

(a) (b)<br />

Figure 2.1: (a) WMAP 5 year CMB temperature anisotropies map from Hinshaw <strong>et</strong> al. (2008); (b) CMB<br />

temperature power spectrum from the WMAP 5 year datas<strong>et</strong> (Nolta <strong>et</strong> al. 2008), along with results from<br />

ACBAR (Reichardt <strong>et</strong> al. 2008), BOOMERANG (Jones <strong>et</strong> al. 2006) and CBI (Readhead <strong>et</strong> al. 2004).<br />

The red curve is the best-fit ΛCDM mo<strong>de</strong>l to the WMAP data.<br />

The most recent CMB measurements come from the WMAP satellite (Komatsu <strong>et</strong> al. 2008),<br />

whose 5 year results for a few ΛCDM param<strong>et</strong>ers, combined with BAO (§ 2.2) and SNe (§ 2.3)<br />

data, are expressed in Table 2.1. In the near future, a new generation of ground and space (like<br />

the Planck satellite (The Planck Collaboration 2006)) experiments will further study the CMB<br />

with even higher accuracy, searching e.g. for the imprint of primordial gravitational waves in<br />

its polarization power spectrum.<br />

Param<strong>et</strong>er WMAP+BAO+SN<br />

t0 13.73 ± 0.12<br />

H0 70.1 ± 1.3<br />

Ωb 0.0462 ± 0.0015<br />

Ωc 0.233 ± 0.013<br />

ΩΛ 0.721 ± 0.015<br />

1.0052 ± 0.0064<br />

Ω0<br />

Table 2.1: Some ΛCDM param<strong>et</strong>ers inferred from the 5 year WMAP+BAO+SN. From Komatsu <strong>et</strong> al.<br />

(2008).<br />

2.2 Large Scale Structure<br />

The various forms of structures (stars, galaxies, clusters of galaxies) we observe today in the<br />

universe (Fig. 2.2), are collectively referred to as the large-scale structure (LSS). They are the<br />

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