Scale and shape dependent non-Gaussianity in the presence of inflationary vector fields
arXiv:1405.7374 · doi:10.1103/PhysRevD.90.103511
Abstract
We consider cosmological inflationary models in which vector fields play some role in the generation of the primordial curvature perturbation . Such models are interesting because the involved vector fields naturally seed statistical anisotropy in the primordial fluctuations which could eventually leave a measurable imprint on the cosmic microwave background fluctuations. In this article, we estimate the scale and shape dependent effects on the non-Gaussianity (NG) parameters due to the scale dependent statistical anisotropy in the distribution of the fluctuations. For concreteness, we use a power spectrum (PS) of the fluctuations of the quadrupolar form: , where is the only quantity which parametrizes the level of statistical anisotropy and is a unitary vector which points towards the preferred direction. Then, we evaluate the contribution of the running of on the NG parameters by means of the formalism. We focus specifically on the details for the NG parameter, associated with the bispectrum , but the structure of higher order NG parameters is straightforward to generalize. Although the level of statistical anisotropy in the PS is severely constrained by recent observations, the importance of statistical anisotropy signals in higher order correlators remains to be determined, this being the main task that we address here. The precise measurement of the shape and scale dependence (or running) of statistical parameters such as the NG parameters and the statistical anisotropy level could provide relevant elements for model building and for the determination of the presence (or nonpresence) of inflationary vector fields and their role in the inflationary mechanism.
arXiv commentLaTex file, 19 pages, 14 figures. v2: the title has been changed a bit to reflect, in a better way, the purpose and contents of the paper. Just a few changes to satisfy the referee requirements. Conclusions unchanged. Version to be published in Physical Review D
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