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STRUCTURE FORMATION MATTEO VIEL INAF and INFN Trieste
SISSA LECTURE nr th March 2011
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OUTLINE: LECTURES Structure formation: tools and the high redshift universe The dark ages and the universe at 21cm IGM cosmology at z=2=6 IGM astrophysics at z=2-6 5. Cosmological probes LCDM scenario 6. Review of main concepts
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GOING NON-LINEAR UNIVERSAL MASS CONSERVATION MAPPING
MEAN CORR FUNCTION WITHIN R INITIAL NEW While non-linear ~ a3 For larger x UNIVERSAL MASS CONSERVATION MAPPING OF LINEAR INTO NON-LINEAR
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GOING NON-LINEAR-I
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COSMIC EXPANSION
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Measuring the cosmic expansion?
This is a fundamental quantity not related at all to the FRW equations! If you want to do such a thing then…
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COsmicDynamicEXperiment CODEX-I
Ultra-stable spectrograph Dz/Dt (10-10 yr-1) REDSHIFT
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CODEX and cosmology -II
Liske et al., 2007, in preparation
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CODEX and cosmology-III
CODEX only no priors CODEX only assuming flatness cosmological constant ± 2 km/s/Mpc and d Wm = 1% 100 yrs 30 yrs 10 yrs w = -1 w = w0 + w a ( 1 - a )
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NON – LINEAR EVOLUTION OF COSMIC STRUCTURE
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LECTURE # 1 Neutralino DM
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Extrapolating a bit…. !!!
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LECTURE # 2 21 cm cosmic structures
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How would the universe at z~12 look like - III?
LCDM DARK ENERGY Gas overdensity Radio sky much brighter than CMB Neutral hydrogen fraction SKY AND FREQUENCY INFORMATION
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LECTURE # 3 NEUTRINOS and LYMAN-a
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Active neutrinos - VIII
Seljak, Slosar, McDonald, 2006, JCAP, 0610, 014 normal 3 1,2 inverted 2 3 1 2s limit Tight constraints because data are marginally compatible mn (eV) < 0.17 (95 %C.L.), < 0.19 eV (Fogli et al. 08) r < 0.22 (95 % C.L.) running = ± 0.012 Neff = 5.2 (3.2 without Ly a) CMB + SN + SDSS gal+ SDSS Ly-a Goobar et al. 06 get upper limits 2-3 times larger…… for forecasting see Gratton, Lewis, Efstathiou 2007
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LECTURE # 4 FEEDBACK FROM GALACTIC WINDS
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Springel & Hernquist 2002,2003
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LECTURE # 5 BAO
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Cosmological parameters from baryonic oscillations
Baryonic acoustic oscillation in SDSS galaxy power spectrum detected in Dec 2004 46748 LRG in 0.72 (Gpc/h)3 at <z>= Eisenstein et al., 2005, ApJ, 633,560 - They are a standard ruler and a signature of the photons-baryons interaction in the the plasma at recombination (z=1100) and provide measurement of H (z) and DA (z) - These soundwaves could either be seen in the CMB peaks or in the galaxy powerspec. with the complication of: bias (galaxy-matter) and peculiar velocities Physical length depends on the sound horizon at recombination DM is angular diameter distance - from CMB DV = [DM2 cz/H(z)] 1/ distance - from LRG dilation scale of the correlation function Different Wm h2
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