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Non-Gaussianity: from Inflation to CMB anisotropies

Non-Gaussianity: from Inflation to CMB anisotropies. Nicola Bartolo Dipartimento di Fisica G. Galilei, Padova, Italy. Plan of the talk. Large-scale CMB anisotropies and primordial NG (second-order radiation transfer function for large-scales). . CMB Anisotropies on all scales:

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Non-Gaussianity: from Inflation to CMB anisotropies

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  1. Non-Gaussianity: from Inflation to CMB anisotropies Nicola Bartolo Dipartimento di Fisica G. Galilei, Padova, Italy

  2. Plan of the talk Large-scale CMB anisotropies and primordial NG (second-order radiation transfer function for large-scales)  CMB Anisotropies on all scales: Boltzmann equations at second-order  Conclusions  - B. N., Matarrese S., Riotto A., Komatsu E., 2004 Phys. Rept. 402, 103 - B. N., Matarrese S., Riotto A., 2004, Phys. Rev. Lett. 93,231301 - B. N., Matarrese S., Riotto A., 2005, JCAP 0508, 010 - B. N., Matarrese S., Riotto A., 2005, JCAP 0605, 24 - B. N., Matarrese S., Riotto A., 2006, JCAP 0606, 24 - B. N., Matarrese S., Riotto A., 2006, astro-ph/0610110 Based on:

  3. Motivations Planck and future experiments may be sensitive to non-Gaussianity (NG) at the level of second- or higher order perturbation theory Crucial to provide accurate theoretical predictions for the statistics of the CMB anisotropies Fundamental: a) what is the relation between primordial NG and non-linearities in the CMB anisotropies on different angular scales? b) what is the non-linear dynamics of the baryon-photon fluid and CDM+ gravity near recombination?

  4. Large-angular scales 3 main effects: a) Sachs-Wolfe effect b) Early and late Integrated Sachs-Wolfe c) Tensor contributions In this limit we do not really need to solve the Boltzmann equations. The relevant effects comes from gravity (at the last scattering surface and from the scattering surface to the observer).

  5. Second-order Sachs-Wolfe effect B. N., Matarrese, Riotto, Phys. Rev. Lett. 2004 gravitational potential at emission specifies the level of primordial non-Gaussianity which depends on the particular scenario for the generation of perturbations Such an expression allows to single out the non-linearities of large-scale CMB anisotropies at last scattering . Evolving them inside the horizon requires the full radiation transfer function at second-order in the perturbations

  6. Fully non-Linear Sachs Wolfe effect  Non-linear perturbations a la Salopek-Bond (1990) definition of the non-linear  quantity  Non-perturbative extension of the Sachs-Wolfe effect N.B., S. Matarrese, A. Riotto JCAP 2005 Linear order Second order see expression in N.B. , Komatsu, Matarrese, Riotto (2004)

  7. The value of (2) is different for different scenarios Post-inflationary nonlinear gravitational dynamics is common to all scenarios From primordial NG to CMB anisotropies • Evaluate the non-Gaussianity generated during inflation (or immediately after as in the curvaton scenario): primordial “input’’ • After inflation, follow the evolution of the non-linearities on large scales by matching the conserved quantity (2) to the initial input, plus Einstein equations at second-order: non-linearities in the gravitational potentials  The non-linearities in the gravitational potentials are then transferred to the observable T/T fluctuations: additional non-linearities are acquired

  8. Sachs-Wolfe effect: a compact formula Initial conditions set during or after inflation Post-inflation non-linear evolution of gravity: order unity NG standard scenario curvaton scenario N.B., Matarrese, Riotto, Phys. Rev. Lett. (2004)

  9. Extracting the non-linearity parameter fNL Connection between theory and observations This is the proper quantity measurable by CMB experiments, via the phenomenological analysis by Komatsu and Spergel (2001) k = | k1 + k2 |

  10. Primordial non-Gaussianity Standard single field models(Maldacena (2002), Acquaviva, Bartolo, Matarrese & A.R. (2002), Lidsey and Seery (2004)) Multiple field models(Kofman (1990+), Bartolo et al., Bernardeau & Uzan (2002+), Rigopoulos, Shellard and Van Tent (2003+), Rigopoulos, (2003+), Lyth, Wands, Malik, Vernizzi (2004+)) Curvaton models and or modulated perturbations(Lyth, Ungarelli and Wands (2002); Bartolo, Matarrese and A.R. (2004); Lyth, Rodriguez, Malik (2005+)) From preheating(Enqvist et al. (2004+), Barnaby and Cline 2006)) Ghost (Arkani-Hamed et al. (2003)) and DBI inflation (Silverstein and Tong (2003)) may be either tiny, or moderate or very large

  11. Inflation models and fNL N. B., E. Komatsu, S. Matarrese and A.Riotto., Phys. Rept. 2004 model fNL(k1,k2) comments Standard inflation K universal, goes to zero in squeezed limit -1/6 +K(k1,k2) curvaton -11/6 - 5r/6 + 5/4r+K(k1, k2) r ~ (rs/r)decay modulated I = - 5/2 + 5G / (12 aG1) I = 0 (minimal case) 1/12 – I +K(k1, k2) order of magnitude estimate of the absolute value may be large ? multi-field inflation “unconventional” inflation set-ups second-order corrections not included Warm inflation typically 10-1 post-inflation corrections not included ghost inflation - 140 b a-3/5 post-inflation corrections not included DBI - 0.1 g2

  12. Angular decomposition The linear and non-linear parts of the temperature fluctuations correspond to a linear Gaussian part and a non-Gaussian contribution At linear order Initial fluctuations Linear radiation transfer function Ex: Linear Sachs-Wolfe Linear ISW

  13. 2nd-order radiation transfer function on large-scales Express the observed CMB anisotropies in terms of the quadratic curvature perturbations with the gravitational potential at last scattering, and are convolutions with kernels and generalize the radiation transfer function at second-order

  14. 2nd-order transfer functions for the Sachs-Wolfe Primordial NG Non-linear evolution of the gravitational potentials after Inflation and additional 2nd-order corrections to temperature anisotropies

  15. 2nd-order transfer functions for the late ISW growth suppression factor Primordial NG Non-linear evolution of the gravitational potentials after inflation Additional second-order corrections to temperature anisotropies (ISW)2 Expression for 2nd-order Early ISW, vector and tensor modes available as well in B. N., Matarrese S., Riotto A., 2005, JCAP 0605

  16. On large scales: NG = NG from gravity (universal)+ NG primordial • Gravity itself is non-linear • Non-linear (second-order) GR perturbations in the standard cosmological model introduce some order unity NG: •  we would be in trouble if NG turned out to be very close • to zero • such non-linearities have a non-trivial form: their computation  core of the (large-scale) radiation transfer function at second-order

  17. WHAT ABOUT SMALLER SCALES ? Aim: - have a full radiation transfer function at second-order for all scales - in particular: compute the CMB anisotropies generated by the non-linear dynamics of the photon-baryon fluid for subhorizon modes at recombination (acoustic oscillations at second-order) Remember: crucial to extract information from the bispectrum are the scales of acoustic peaks according to the phenomenological analysis of Komatsu and Spergel (2001)

  18. 2nd-order CMB Anisotropies on all scales Apart from gravity account also for: a) Compton scattering of photons off electrons b) baryon velocity terms v Boltzmann equation for photons Collision term Gravity effects + Boltzmann equations for baryons and CDM+ Einstein equations

  19. Metric perturbations Poisson gauge i and ij second-order vector and tensor modes. Examples: using the geodesic equation for the photons Redshift of the photon (Sachs-Wolfe and ISW effects) Direction of the photons changes due to gravitational potentials Lensing effect (it arises at second-order) PS: Here the photon momentum is ; ( quadri-momentum vector)

  20. Photon Boltzmann equation Expand the distribution function in a linear and second-order parts around the zero-order Bose-Einstein value Left-hand side

  21. The collision term C[f] Crucial points to compute the second-order collision term: 1) Little energy /T is transferred expand in the perturbations and in /T  q/me. At linear order the Boltzmann equations depend only on ni, at second-order there is energy exchange (p dependence) and thus spectral distorsions. 2) Take into account second-order baryon velocity v(2) 3) Take into account vortical components of (first-order  first-order)  Up to recombination photons are tightly coupled to electrons via Compton scatterings e(q) (p)  e(q’) (p’). The collision term governs small scale anisotropies and spectral distorsions   Important also for secondary scatterings: reionization, kinetic and thermal Sunyaev-Zeldovich and Ostriker-Vishniac effects

  22. The 2nd-order brightness equation Second-order baryon velocity Sachs-Wolfe effects Gravitational lensing Quadratic-Doppler effect Coupling velocity and linear photon anisotropies with optical depth Source term

  23. Hierarchy equations for multipole moments Free-streeming of photons: Suppression of anisotropies From . It gives a projection effect of inhomogeinities onto anisotropries At linear order responsible of the hierarchy Residual scattering effects and gravity and Expand the temperature anisotropies in multipole moments System of coupled differential equations

  24. Integral Solution and One can derive an integral solution in term of the Source Important: The main information is contained in the Source, which contains peculiar effects from the non-linearity of the perturbations   The integral solution is a formal solution (the source contains second-order moments up to l=2), but still more convinient than solving the whole hierarchy

  25. CMB anisotropies generated at recombination KEY POINT: Extract all the effects generated at recombination (i.e. Isolate from the Source all those terms  optical depth ’ ) Visibility function sharply peaks at recombination epoch *

  26. Need to know the evolution of the photon energy density (2)00 , velocity and gravitational potentials around recombination Yields anisotropies generated at recombination due to the non-linear dynamics of the photon-baryon fluid

  27. example:  Collision terms: electrons are coupled to protons via Coulomb scatt. driving e=p=b and ve= vp v (“baryons”); + Compton scatterings e Boltzmann equations for massive particles The Source term requires to know the evolution of baryons and CDM Left-hand side :  just extend to a massive particle with mass m and energy E=(m2+q2)1/2

  28. Momentum continuity equation Photon velocity 2nd-order velocity Quadrupole moments of photon distribution

  29. Acoustic oscillations at second-order In the tight coupling limit the energy and momentum continuity equations for photons and baryons reduce to

  30. 1) At second-order vector perturbaztions are inevitably generated The quadrupole moment at recombination Two important differences w .r. s to the linear case: 2) At second-order the quadrupole of the photons is no longer suppressed in the tight coupling limit Similar term analyzed by W. Hu in ApJ 529 (2000) in the context of reionazation

  31. Non-linear dynamics at recombination Modes entering the horizon during the matter epoch (-1* < k < -1EQ) Acoustic oscillations of primordial non-Gaussianity Non-linear evolution of gravity

  32. Linear vs. full radiation transfer function primordial non-Gaussianity is transferred linearly:Radiation Transfer function at first order Non-linear evolution of gravity: the core of the 2nd order transfer function (how these contributions mask the primordial signal? how do they fit into the analysis of the bispectrum?) Numerical analysis in progress (N.B., Komatsu, Matarrese, Nitta, Riotto) (from Komatsu & Spergel 2001)

  33. Modes entering the horizon during radiation epoch (k > -1EQ ) In this case the driving force is the quadrupole

  34. Modes entering the horizon during radiation epoch (II): The Meszaros effect Around the equality epoch EQ Dark Matter starts to dominate Consider the DM perturbations on subhorizon scales during the radiation epoch Meszaros effect: This allows to fix the gravitational potential at  >EQ through the Poisson equation and to have a more realistic and accurate analytical solutions for the acoustic oscillations from the equality onwards

  35. Meszaros effect at second-order Combining the energy and velocity continuity equations of DM for a R.D. epoch Solution Initial conditions:

  36. fix the initial conditions for the evolution of the gravitational potential and photons perturbations at  >EQ for subhorizon modes Interesting for NG and Large Scale Structure studies: determine the full second-order transfer function for matter perturbations(primordial non-Gaussianity parametrized by aNL is transferred linearly, but the core of the transfer function is given by the remaining terms). See N.B, Matarrese & Riotto, JCAP2222, for the case of modes entering the horizon after equality  Meszaros effect at second-order Dark Matter density contrast on subhorizon scales for  < EQ Can be used for two pourposes:

  37. Second-order transfer function First step: calculation of the full 2-nd order radiation transfer function on large scales (low-l), which includes: • NG initial conditions • non-linear evolution of gravitational potentials on large scales • second-order SW effect (and second-order temperature fluctuations on last-scattering surface) • second-order ISW effect, both early and late • ISW from second-order tensor modes (unavoidably arising from non-linear evolution of scalar modes), also accounting for second-order tensor modes produced during inflation Second step: solve Boltzmann equation at 2-nd for the photon, baryon and CDM fluids,which allows to follow CMB anisotropies at 2-nd order at all scales; this includes both scattering and gravitational secondaries, like: • Thermal and Kinetic Sunyaev-Zel’dovich effect • Ostriker-Vishniac effect • Inhomogeneous reionization • Further gravitational terms, including gravitational lensing (both by scalar and tensor modes), Rees-Sciama effect, Shapiro time-delay, effects from second-order vector (i.e. rotational) modes, etc. … In particular we have computed the non-linearities at recombination (Bartolo, Matarrese & A.R. 2005+)

  38. Conclusions Up to now a lot of attention focused on the bispectrum of the curvature Perturbation . However this is not the physical quantity which is observed is (the CMB anisotropy)  Need to provide an accurate theoretical prediction of the CMB NG in terms of the primordial NG seeds  full second-order radiation transfer function at all scales  Future techniques (predicted angular dependence of fNL, extensive use of simulated NG CMB maps, measurements of polarization and use of alternative statistical estimators ) might help NG detection down to fNL~1: need to compute exactly the predicted amplitude and shape of CMB NG from the post-inflationary evolution of perturbations. 

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