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Cosmology from Large Scale Structure Surveys
Changbom Park Feb. 27, School of Physics Korea Institute for Advanced Study
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A sketch of Astronomer's methods to measure cosmological parameters (DE's w)
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『What we want to know』 1. Spacetime 2. Matter 3. Phenomena/Laws
Homogeneous & isotropic space Geometry & topology of space (flat & infinite?) Expansion of space ( matter) Past and future of the Universe (why now?) 2. Matter Contents and nature (what & how much) Primordial fluctuation () Structure formation (when & how, environment) 3. Phenomena/Laws
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the Uni-verse: a map of our play-ground
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1. Recombination & Decoupling
Dark First NL Evolution LSS hear & now age structures of galaxies 1. Recombination & Decoupling CMB radiation. Let there be primeval light ! 2. Dark Age What is buried here? 2. First structures & Reionization Let there be star light ! 4. High-z objects and Evolution of galaxies Quasars, Ly-a forest clouds 5. Large-scale structure and nearby objects Cosmic zoo: clusters, voids, filaments & walls of galaxies Recent events in the universe
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Expansion of space & Growth of structures
Ideas to draw information on the universe 1. Look at primordial fluctuations directly CMB (+neutrino, gravitational wave) => geometry of space, matter contents, matter P(k), non-Gaussianity 3. Study the expansion history of the space : H(t) or r(z) use standard candle (SN Ia), rulers (BAO, topology) => matter contents (DE w) 4. Measure the growth of structures use gravitational lensing, cluster abundance depends on expansion of space, matter power spectrum 5. Study the properties of non-linear structures properties of galaxies, clusters Expansion of space & Growth of structures
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Cosmic microwave background anisotropy:
CMB anisotropy: Primordial & ISW Cosmic microwave background anisotropy: geometry of space, matter contents, matter P(k), non-Gaussianity only at z~1100, 2d map, foregrounds
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WMAP Experiment WMAP Observatory
Launched on 30 June 2001 to L2 of Sun-Earth system 1.4m*1.6m primary + 10 feed horns in each 2 focal plane Bands 1 K 1 Ka 2 Q 2 V 4 W Ν [GHz] 22.8 33 40.7 60.8 93.5 FWHM [°] 0.82 0.62 0.49 0.33 0.21
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Observed ΔT Maps W 94GHz 0.21° V 61GHz 0.33° Q 41GHz 0.49°
K 23GHz 0.82° Ka 33GHz 0.62° Galactic emission + CMBR + others
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WMAP's 3 year Map Park, Park, Gott (2007)
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Spergel et al. (2007) 3yr & 1yr data 3yr & 1yr fits
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Shape of T Power Spectrum
Super-horizon scale fluc. SW effect 1∼0.1rH fluc. with initially coherent phases Oscillation & Doppler effect Radial averaging & radiation diffusion
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Spergel et al. (2007) 3yr & 1yr constraints
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Park, Park, Gott (2007)
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HI HI HI HI HI HI HI HI HI HI HI HI HI HI HI HI 3D HI distribution & reionization
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3D HI distribution : 21cm tomography mapping most of our observable universe
Power spectrum of 21cm fluctuations HI HI HI HI HI HI HI HI HI HI HI HI HI HI Bright in HI !
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Gravitational Lensing: Strong & Weak
only projected mass along the line of sight
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Shear map expected in SCDM
Jain, Seljak & White (2000) mass fluctuations along the line of sight >Weak lensing by LSS > coherent distortions in the observed shapes of background galaxies Shear map expected in SCDM
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CFTHLS weak-lensing survey: i<24.5 & 22 deg2
Spergel (2007)
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Type Ia Super Novae Intrinsic dispersion, systematics
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r(z) relation : Expansion history
SN Ia as a standard candle Transition from deceleration to acceleration at z= 0.46 ± 0.13 (Riess et al. 2004)
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μ = m-M = 5log dl + 25 Ωm=0.27, ΩΛ=0.73 Riess et al. (2007)
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Matter contents Dark energy Ωm=0.29±0.050.03, ΩΛ=0.71 (if flat U)
(Riess et al. 2004) (Riess et al. 1998) (Riess et al. 2004) Matter contents Ωm=0.29± , ΩΛ=0.71 (if flat U) Dark energy w = -1.02± , w<-0.76 at 95% (if P=wρc2)
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Clusters
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Clusters of galaxies Searched by X-ray, SZ effect abundance d2N/dMdz
spatial distribution P(k)
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Future experiments clusters CMB SN Ia
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Large Scale Structure in linear ~ quasi-linear regime : P(k), BAO, Topology
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Geometric methods using the large scale structures
Standard rulers (Actual objects or Features in PS/CF) measure Δz & Δθ H(z)DA(z) Ωm, ΩΛ, w (=dt/a) r|| r┴ (=r dθ) where H(z)
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BAO (ex) Features in PS & CF Baryonic oscillation in PS
Baryonic bump in CF of deep redshift sample Ωm, ΩΛ, w We know actual length! Acoustic oscillation : amplitude depends on Ωb scale = comoving sound horizon ‘s’ at last scattering kA = 2π/s depends strongly on Ωm, weakly on Ωb not on DE Curvature of space, Baryonic mass
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SDSS DR5 Best fit m=0.26 (Percival et al. 2007)
Main galaxies and LRGs BAO+HST h=0.72 BAO+WMAP3 Best fit m=0.26
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Power Spectrum from CMB & LSS : Ωm
But biasing relative to matter
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Linear scale structures do not change shape
(Springel) Linear scale structures do not change shape Intrinsic topology of LSS insensitive to biasing & redshift distortion
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LSS topology as a standard ruler
Primordial density Dark matter at z=0 LSS topology as a standard ruler Dark halos at z=0 in r Dark halos at z=0 in z 25h-1Mpc Gaussian smoothing
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Cosmological parameter estimation from LSS topology
curvature in P(k) => genus(λ) depends on cosmology Inconsistency test ! given z => choose a cosmology, i.e. r(z) => measure genus(λ) => compare model prediction & measurement of genus
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Constraint on Ωm better than WMAP3
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Properties of non-linear structures
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? LSS CMBR 70s BB+(γ,ν; baryon)+GI Dark matter 82Inflation
80s CMBR dT/T < 10-4 Late70s Discovery of LSS mid80 SCDM Model BB+Inflation+(γ,ν; baryon, CDM)+GI 92 COBE dT/T~10-5 92 LSS P(k) SCDM Model ruled out 98 Accelerating expansion WMAP Cℓ >2000 Concordance LCDM Model BB+Inflation+(γ,ν; baryon, CDM; Dark E)+GI SDSS JWST many more Planck ? Topology of space; matter contents; matter fluctuation & structure formation
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Small scale 1/√N reduction
Decoupling surface Acoustic oscillation Small scale 1/√N reduction & Photon diffusion Width Δz=195 Δr=44Mpc 1. Inflation Same initial phase of oscillation peaks & troughs in PS 2. Baryonic λJb 2200Mpc ≫ Horizon rHdec 320Mpc > Sound horizon λs 270Mpc > Width Δr 44Mpc > Photon Diffusion λD 14Mpc
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3. Gaussianity of ΔT/T Minkowski functionals
G(ν)=(Nhot-Ncold)/2πA Gaussian: No frequency, scale dependence ! Non-Gaussianity Detected! (Park & Park 03)
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