Primordial non-Gaussianity from multifield DBI Galileons

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Presentation transcript:

Primordial non-Gaussianity from multifield DBI Galileons SI2011 @ Fujiyoshida 2011. 8. 4 Primordial non-Gaussianity from multifield DBI Galileons Shuntaro Mizuno ICG, Portsmouth APC and LPT, Paris S. Renaux-Petel, S.M, K. Koyama arXiv:1108.0305 [astro-ph.CO]

DBI inflation A natural inflation model based on string theory which can generate large equilateral NG Silverstein, Tong `04 Inflation is identified as a radial position modulus of a probe D3 brane in extra-dimensions small sound speed enhances NG 6D Calabi-Yau D3 Single field model in string theory inflaton is severely constrained anti-D3 Lidsey, Huston `07 Kobayashi, Mukohyama, Kinoshita `07

Multifield DBI inflation DBI inflation is naturally a multifield model (Angular directional coordinates) Easson, Gregory, Tasinato, Zavala `07 Multifield effect can ease the problem background trajectory    same momentum dependence entropy    Langlois, Renaux-Petel, Steer, Tanaka `08 adiabatic     Arroja, Mizuno, Koyama `08 Trispectrum momentum dependence is different from single field model easier to detect if there is large transfer Arroja, Mizuno, Koyama, Tanaka `09 Mizuno, Arroja, Koyama, Tanaka `09

DBI Galileon Natural unification of DBI and Galileon A probe brane dynamics in 5D de Rham, Tolley `10 Induced metric of the brane y Extrinsic curvature of the brane brane is localised at Lorentz factor Requiring E.O.Ms are kept to be second order DBI Relativistic extension of Galileon

Non-Gaussianity from single field DBI Galileon Simplest extension of single field DBI inflation Mizuno, Koyama `10 with standard DBI ( ) L ( ) L 2 3 almost independent of Related works for NG from single field Galileon models Kobayashi, Yamaguchi, Yokoyama `11 general Burrage et al `10 all terms satisfying exact Galileon symmetry De Felice, Tsujikawa `11 further generalised model

1. Motivations 2. Model and background 3. Linear perturbations 4. Non-Gaussianity 5. Conclusions

DBI Galileon with higher co-dimensions ・ Induced metric , L If we require the action to be scalar with respect to I, only tension and scalar curvature can be allowed!! 2 L L L 3 4 5 Furthermore, it was shown that for even codimensions with the only possible term is the induced gravity term ( ) Hinterbichler, Trodden, Wesley `10 cf. Matching condition for a brane of arbitrary codimensions Charmousis, Zegers `05

Model ・ Embedding a brane in 10-dimensions Renaux-Petel, Mizuno, Koyama `11 ・ Embedding a brane in 10-dimensions warp factor ・ Induced metric on the brane with ・ Action with

Equations of motion Including dependence Christoffel symbol associated with ………..

Cosmological background ・ Friedmann equation ・ In the relativistic regime ( ), the induced gravity gives a term that breaks the null energy condition ・ Condition for inflation in the relativistic regime with

Linear perturbations ・ Second-order action ・ No ghost instabilities entropy    ・ Sound speeds adiabatic     Entropic sound speed is smaller than adiabatic one (they become same in the DBI inflation )

Non-Gaussianity ・ Third-order action ・ Bispectrum with adiabatic entropy induced     for standard DBI inflation     

Momentum dependence of Bispectrum ・ For the fast analysis of NG from the bispectrum, separable theoretical templates are used. ・ Equilateral shape ・ Orthogonal shape ( absolute value)      ・ Constraints Fergusson, Shellard `10

Correlation of the adiabatic shape (relativistic limit ) ・ vs equilateral template ・ vs orthogonal template Mostly it gives equilateral NG but for a narrow region of , it gives orthogonal type NG !

Correlation of the entropic-induced shape (relativistic limit ) ・ vs equilateral template ・ vs orthogonal template Qualitatively similar to the adiabatic shape , but value of which gives orthogonal type NG is different

Observational constraint ・ No entropic transfer ・ Large entropic transfer log log

Conclusion Multifield DBI Galileon a probe brane action with an induced gravity Relativistic inflation can be realised if Cosmological perturbations are controlled by two parameters ghost condition is specified sound speeds and are different constraints on these parameters for given concrete example to give orthogonal type NG and positive

Discussions Entropy transfer Concrete model ( ) New shape from general multifield model general cosmological background Trispectrum

Multi-field non-Gaussianity (new-effect) ・ Bispectrum shape generated by k2/k1 k2/k1 k3/k1 k3/k1 ``Equilateral” ``local” location of the maximum changes from Equilateral to local !!

Concrete form of