Takahiro Nishimichi (IPMU)
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1 Accurate Modeling of the Redshift-Space Distortions based on arxiv: of Biased Tracers Takahiro Nishimichi (IPMU) with Atsushi Taruya (RESCEU) RESCEU/DENET summer school in Aso, Kumamoto, July
2 Dark Energy? Modified Gravity? observations acceleration of cosmic expansion type-1a supernova BAOs CMB... f(r), DGP,... modified gravity? G µν = 8πG c 4 T µν dark energy? SNLS3, Conley+ 11 expansion history in a DE model may be mimicked by a MG model geometrical + growth tests are essential!
3 Anisotropies in galaxy clustering distance measurements in z-space BAOs + Alcock & Paczynski test power spectrum (normalized) Blake+ 11a WiggleZ Dark Energy Survey wavenumber k [h/mpc] A. Taruya A. Taruya H(z) & DA(z) z-space distiontions f(z) d ln D(z) d ln a Blake+ 11b f σ8 redshift z space real space peculiar velocity
4 Redshift-space distortions z-space r-space r-space peculiar velocity Kaiser Effect large-scale coherent motion enhancement of clustering Finger-of-God Effect small-scale random motion suppression of clustering k μ = 1 μ = 0 k e.g., Scoccimarro 04 streaming model vel. divergence: vel. dispersion: σv
5 Redshift-space distortions z-space r-space r-space peculiar velocity Kaiser Effect large-scale coherent motion enhancement of clustering Finger-of-God Effect small-scale random motion suppression of clustering k μ = 1 μ = 0 k e.g., Scoccimarro 04 streaming model vel. divergence: vel. dispersion: σv
6 Redshift-space distortions z-space r-space z-space r-space peculiar velocity Kaiser Effect large-scale coherent motion enhancement of clustering Finger-of-God Effect small-scale random motion suppression of clustering k μ = 1 μ = 0 k e.g., Scoccimarro 04 streaming model vel. divergence: vel. dispersion: σv
7 Redshift-space distortions z-space r-space r-space peculiar velocity Kaiser Effect large-scale coherent motion enhancement of clustering Finger-of-God Effect small-scale random motion suppression of clustering k μ = 1 μ = 0 k e.g., Scoccimarro 04 streaming model vel. divergence: vel. dispersion: σv
8 Redshift-space distortions z-space r-space r-space peculiar velocity Kaiser Effect large-scale coherent motion enhancement of clustering Finger-of-God Effect small-scale random motion suppression of clustering k μ = 1 μ = 0 k e.g., Scoccimarro 04 streaming model vel. divergence: vel. dispersion: σv
9 Redshift-space distortions z-space r-space z-space r-space peculiar velocity Kaiser Effect large-scale coherent motion enhancement of clustering Finger-of-God Effect small-scale random motion suppression of clustering k μ = 1 μ = 0 k e.g., Scoccimarro 04 streaming model vel. divergence: vel. dispersion: σv
10 Redshift-space distortions (contd.): TNS model Exact formula for the z-space P(k) Taruya, Nishimichi, Saito ( 10) notice e A BC e A BC with a help of cumulant expansion theorem monopole w/o correction A term cross-bispectrum of δ & θ new terms! quadrupole B term sum of convolutions of Pδθ & Pθθ
11 Redshift-space distortions (contd.): TNS model Exact formula for the z-space P(k) Taruya, Nishimichi, Saito ( 10) notice e A BC e A BC with a help of cumulant expansion theorem monopole w/o correction w/ correction A term cross-bispectrum of δ & θ new terms! quadrupole B term sum of convolutions of Pδθ & Pθθ
12 RSDs for biased tracers? Many people are working hard on this! Okumura & Jing 11 e.g., Okumura & Jing 11 Tang, Kayo & Takada 11 Reid & White 11 Sato & Matsubara 11 biased tracer? assume δg = bδ k [h/mpc] k [h/mpc] β = f / b A term cross-bispectrum of δ & θ B term sum of convolutions of Pδθ & Pθθ Are correction terms enhanced by bias?
13 Analysis Large N-body simulations (L=1.14Gpc/h, N=1,280 3 ) starting with 2LPT initial conditions x 15 realizations 9 halo catalogs over a wide mass z=0.35 volume & number density SDSS DR7 LRGs b(k) is directly measured from r-space clustering σv is treated as a free fitting parameter mass: h -1 Msun, density: h 3 Mpc -3 k [h/mpc]
14 Result N-body simulations dark matter light halos heavy halos
15 dark matter light halos heavy halos Result TNS model dark matter light halos heavy halos
16 dark matter light halos heavy halos Result streaming TNS model model dark matter light halos heavy halos
17 dark matter light halos heavy halos Result streaming TNS model model dark matter light halos heavy halos
18 Goodness of fits best-fit values of σv: smaller for streaming model consistent with 0 for massive halos consistent with the linear theory for TNS does not depend the halo mass FoG function: Lorentzian (L), Gaussian (G) goodness of fit: worse for streaming model especially for massive halos reduced χ 2 are close to 1 for TNS independent of the halo mass
19 Recovery of f(z) 2 parameter fit to N-body data: f and σv streaming model seams OK only at kmax<0.1h/mpc typically ~5% underestimate of f TNS model gives unbiased estimate of f up to kmax ~ 0.2 h/mpc
20 Recovery of f(z) 2 parameter fit to N-body data: f and σv streaming model seams OK only at kmax<0.1h/mpc typically ~5% underestimate of f TNS model gives unbiased estimate of f up to kmax ~ 0.2 h/mpc
21 Recovery of f(z) 2 parameter fit to N-body data: f and σv streaming model seams OK only at kmax<0.1h/mpc typically ~5% underestimate of f TNS model gives unbiased estimate of f up to kmax ~ 0.2 h/mpc
22 Recovery of f(z) 2 parameter fit to N-body data: f and σv streaming model seams OK only at kmax<0.1h/mpc typically ~5% underestimate of f TNS model gives unbiased estimate of f up to kmax ~ 0.2 h/mpc
23 Recovery of f(z) 2 parameter fit to N-body data: f and σv streaming model seams OK only at kmax<0.1h/mpc typically ~5% underestimate of f TNS model gives unbiased estimate of f up to kmax ~ 0.2 h/mpc
24 Recovery of f(z) 2 parameter fit to N-body data: f and σv streaming model seams OK only at kmax<0.1h/mpc typically ~5% underestimate of f TNS model gives unbiased estimate of f up to kmax ~ 0.2 h/mpc
25 Future/on-going surveys Fisher matrix analysis with 5 parameters (b, σv, H, DA, f) Assumption TNS model is true, but adopt streaming model h -3 Gpc 3 h 3 Mpc -3 h Mpc -1 f(z) = [Ω m (z)] γ γ =0.77 ± 0.04
26 Summary tested the clustering of halos in z-space by N-body simulations... frequently used phenomenological model is not sufficient ~5% systematic bias in f(z) correction terms in TNS model more prominent for more massive halos or more biased objects codes for our model are publicly available!! visit CPT library:
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