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The influence of Dark Energy on the Large Scale Structure Formation

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Presentation on theme: "The influence of Dark Energy on the Large Scale Structure Formation"— Presentation transcript:

1 The influence of Dark Energy on the Large Scale Structure Formation
Dec The influence of Dark Energy on the Large Scale Structure Formation International Workshop on Dark Matter, Dark Energy, and Matter-Antimatter Asymmetry November. 21th .2009 Seokcheon (sky) Lee Institute of Physics, Academia Sinica & LeCOSPA, NTU

2 Dec Outline 1. Linear perturbation of matter with dark energy when DE is the cosmological constant (Λ) or general DE 1-I. Exact Analytic solution of density perturbations (δ = D) 1-II. Growth index and its parameter (f and γ) 2. Non-linear perturbation of matter (SCM) with(out) curvature 3. Non-linear perturbation of matter with dark energy 4. Observational consequences. 5. Summary Nov.21th.2009 Sky Lee // IWDMDE

3 Dec Observations Nov.21th.2009 Sky Lee // IWDMDE

4 Linear perturbation theory.i
Dec Linear perturbation theory.i Matter distribution in the Universe (Large scale) : Homogeneous Contains inhomogeneous structures (Small scale) : galaxies, clusters A small inhomogeneity grows due to gravitational instability At late times (z < 10), all interesting modes enter the horizon : sub-horizon scale(s) Nov.21th.2009 Sky Lee // IWDMDE

5 Linear perturbation theory.ii
Dec Linear perturbation theory.ii Uniform growth (independent of k) due to the pressure-less DM : all modes evolves identically Figures from : Ma et.al. [arXiv:astro-ph/ ] Nov.21th.2009 Sky Lee // IWDMDE

6 LPT Equations Perturbed equations Dec.02.2008 Nov.21th.2009
Sky Lee // IWDMDE

7 Dec Solve LPT 1. Numerical method : need to separate both the growing mode and decaying mode from 2. Analytic method : only true for cosmological constant or curvature with integral form. Nov.21th.2009 Sky Lee // IWDMDE

8 Analytic solution i-a For cosmological constant or curvature term
Dec Analytic solution i-a For cosmological constant or curvature term Growth factor Growth index and its parameter Nov.21th.2009 Sky Lee // IWDMDE

9 Dec Analytic solution i-b Peculiar velocity : ~30% differences for matter Nov.21th.2009 Sky Lee // IWDMDE

10 Dec Analytic solution i-c Nov.21th.2009 Sky Lee // IWDMDE

11 Analytic solution ii-a
Dec Analytic solution ii-a Solution for any general dark energy models Growth factor (growing mode solution) Growth index and its parameter Nov.21th.2009 Sky Lee // IWDMDE

12 Analytic solution ii-b
Dec Analytic solution ii-b Nov.21th.2009 Sky Lee // IWDMDE

13 Dec Future Observations Nov.21th.2009 Sky Lee // IWDMDE

14 Dark matter and baryon I
Dec Dark matter and baryon I DM dependence on matter density will confuse with the model dependence. Nov.21th.2009 Sky Lee // IWDMDE

15 Dark matter and baryon II
Dec Dark matter and baryon II Baryon catch up the DM after the decoupling. Quite model independent and unique. If find anti-bias, then good for some coupling model (preparation with G-C Liu and K-W Ng) Nov.21th.2009 Sky Lee // IWDMDE

16 Spherical Collapse Model (SCM)
Dec Spherical Collapse Model (SCM) Nov.21th.2009 Sky Lee // IWDMDE

17 Nonlinear matter perturbation
Dec Nonlinear matter perturbation General method : Spherical collapse model (SCM) with and without curvature term Nov.21th.2009 Sky Lee // IWDMDE

18 SCM with(out) k .I Define new parameters Dec.02.2008 Nov.21th.2009
Sky Lee // IWDMDE

19 Dec SCM with(out) k .II Nov.21th.2009 Sky Lee // IWDMDE

20 SCM with(out) k .III Virial theorem Dec.02.2008 Nov.21th.2009
Sky Lee // IWDMDE

21 SCM with(out) k .IV Linear regime (critical threshold density)
Dec SCM with(out) k .IV Linear regime (critical threshold density) Nov.21th.2009 Sky Lee // IWDMDE

22 Dec SCM with DE .I Nov.21th.2009 Sky Lee // IWDMDE

23 Dec SCM with DE .II Nov.21th.2009 Sky Lee // IWDMDE

24 Dec SCM with DE .III Nov.21th.2009 Sky Lee // IWDMDE

25 Dec SCM with DE .IV Nov.21th.2009 Sky Lee // IWDMDE

26 Observables CMB and Matter Power Spectrum (linear)
Dec Observables CMB and Matter Power Spectrum (linear) Baryonic Acoustic Oscillation (linear + non-linear) SUBARU : Hyper Suprime-Cam (HSC) : ASIAA : Cluster abundances, Weak Lensing (WL), Nov.21th.2009 Sky Lee // IWDMDE

27 Dec Summary Linear perturbation theory in sub-horizon scales important for the structure formation. We are able to obtain the exact values of growth index and exact analytic solution of growth factor for any DE models. This simple and exact solution give the guidelines for future observations (sigma8, etc..) Nonlinear model can be used for probing cluster abundances, mass function, WL, and BAO. Exact solutions provide accurate tools for probing DE. Nov.21th.2009 Sky Lee // IWDMDE


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