lyman alpha forest and primordial non gaussianities fnl
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Lyman-alpha forest and Primordial Non-gaussianities (fnl) with collaborators: Anze Slosar, Uros Seljak and Vincent Desjacques Shirley Ho Lawrence Berkeley Lab 18 Sep 2009, Paris-Berkeley meeting Outline What is fnl? What have we


  1. Lyman-alpha forest and Primordial Non-gaussianities (fnl) with collaborators: Anze Slosar, Uros Seljak and Vincent Desjacques Shirley Ho Lawrence Berkeley Lab 18 Sep 2009, Paris-Berkeley meeting

  2. Outline • What is fnl? • What have we done with LSS and fnl? • What can we do with Lya and fnl? —Lya flux spectra with different non-gaussianities —How about with redshift space distortions? • Things to worry about: —UV background fluctuations —Continuum subtractions ...

  3. Lyman Alpha Forest: what is it? Time z~0 z~6 z~1100 Redshift

  4. Lyman Alpha Forest: what is it? Time z~0 z~6 z~1100 Courtesy simulation of gas from Renyue Cen and Jerry Ostriker Redshift

  5. Lyman Alpha Forest: what is it? Time z~0 z~6 z~1100 Courtesy image from Joanne Cohn’s website Redshift

  6. Lyman Alpha Forest: what is it? Time Flux z~0 z~6 z~1100 λ (˚ A ) Redshift

  7. Lyman Alpha Forest: what is it? Time Flux z~0 Locates the Neutral Hydrogen, thus overdensities of the Universe. z~6 z~1100 λ (˚ A ) Redshift

  8. What is fnl? —Non-gaussianities in Early Universe parameterize how much non-linear corrections are there to the potential Φ = φ + f NL φ 2 Primordial potential (assumed to be gaussian random field) V ( φ ) reheating Inflation

  9. What is fnl? —Non-gaussianities in Early Universe parameterize how much non-linear corrections are there to the potential Φ = φ + f NL φ 2 Primordial potential (assumed to be gaussian random field) V ( φ ) reheating Inflation

  10. Stolen from Ben Wandelt

  11. Stolen from Ben Wandelt

  12. Stolen from Ben Wandelt

  13. Stolen from Ben Wandelt

  14. Stolen from Ben Wandelt

  15. What have we done with LSS and fnl? —Non-gaussianities in Early Universe Slosar et al. 2008 Best current CMB measurement f NL f NL curvaton canonical ghost models, inflation inflation DBI inflation

  16. Lyman Alpha Forest: what can it do?

  17. Lyman Alpha Forest: what can it do? Ω m = 0 . 25 , Ω Λ = 0 . 75 , h = 0 . 75 , n = 0 . 97 , σ 8 = 0 . 8 1024 3 particles, L box = 1 . 6 Gpc/h

  18. Lyman Alpha Forest: what can it do? Ω m = 0 . 25 , Ω Λ = 0 . 75 , h = 0 . 75 , n = 0 . 97 , σ 8 = 0 . 8 1024 3 particles, L box = 1 . 6 Gpc/h Fluctuating Gunn Peterson approximation τ = A (1 + δ ) β F = e − τ

  19. Lyman Alpha Forest: what can it do? • Primordial Non-gaussianities via Lyman alpha forest Skewers of Neutral Hydrogen

  20. Lyman Alpha Forest: what can it do? Skewers of Neutral Hydrogen Take the 3D power-spectrum of these skewers!

  21. P(k) (Mpc/h)^3 k (h/Mpc) Courtesy slide from Anze Slosar

  22. What can we do with Lya and fnl? P f NL 0.4 − 1 fnl = -100 fnl = +100 P f NL =0 0.3 0.2 fnl = -100 P_fnl(k)/P_fnl=0(k) -1 0.1 0 -0.1 fnl = +100 -0.2 -0.3 0.01 0.1 k (h/Mpc) Ho, Slosar, Seljak & Desjacques (in prep)

  23. What can we do with Lya and fnl? P f NL − 1 P f NL =0 With z-space distortions! fnl = -100 (z-space) fnl = +100 (z-space) Ho, Slosar, Seljak & Desjacques (in prep)

  24. What can we do with Lya and fnl? —Non-gaussianities in Early Universe ∆ ( f NL ) ∼ 1 BigBOSS Ly-alpha forest constraints Planck forecasted constraints ∆ ( f NL ) ∼ 5 BOSS LRG only constraints ∆ ( f NL ) = 18 Best current CMB measurement f NL curvaton canonical ghost Ho, Slosar, Seljak & Desjacques (in prep) models, inflation inflation DBI inflation

  25. Other things we should worry about: • UV background fluctuations • continuum subtractions • others? • There maybe easy solutions: —Using multiple tracers! —Quasars, LRGs, Lyman-alpha forest (but in different ways)

  26. Lyman Alpha Forest: what else can it do? • Dark Energy via Baryon Acoustic Oscillations —the correlation function: ξ f ( r ) = < δ f (ˆ x ) δ f (ˆ x + ˆ r ) >

  27. Lyman Alpha Forest: what can it do? • Dark Energy via Baryon Acoustic Oscillations —the correlation function: ξ f ( r ) = < δ f (ˆ x ) δ f (ˆ x + ˆ r ) >

  28. Lyman Alpha Forest: what can it do? • Dark Energy via Baryon Acoustic Oscillations —take the correlation function: r 2 ξ ( r ) What acoustic peak would look like if we use Lya forest flux! ξ f ( r ) = < δ f (ˆ x ) δ f (ˆ x + ˆ r ) > Flux Real (Redshift) Space Correlation function r (h/Mpc) Slosar, Ho, White & Louis (2009)

  29. Lyman Alpha Forest: what can it do? r 2 ξ ( r ) Redshift Space Correlation function Scaled matter correlation functions Real Space Correlation function r (h/Mpc) Slosar, Ho, White & Louis (2009)

  30. Conclusions • We can probe early universe with Lya forest! • z-space distortions? not a problem! • Other things Lya forest can do? —BAO -> Dark energy at high-z —neutrino mass constraints (small scale P(k)) —IGM physics... • We need to worry about systematics such as: —UV background fluctuations —continuum fluctuations, etc

  31. Checking my Lya-P(k) \ kP ( k ) / π

  32. What does fnl do?

  33. What does fnl do?

  34. What about z-space distortions? P(k) [Mpc/h]^3 1.2 z-space distorted flux P(k) fnl=-100 z-space distorted flux P(k) fnl=+100 1.1 1 P_F(k) (Mpc/h)^3 0.9 0.8 0.7 0.6 0.001 0.01 0.1 1 k (h/Mpc) k (Mpc/h)^{-1}

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