2011
DOI: 10.1088/1475-7516/2011/06/026
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Bispectra from two-field inflation using the long-wavelength formalism

Abstract: We use the long-wavelength formalism to compute the bispectral non-Gaussianity produced in two-field inflation. We find an exact result that is used as the basis of numerical studies, and an explicit analytical slow-roll expression for several classes of potentials that gives insight into the origin and importance of the various contributions to f NL . We also discuss the momentum dependence of f NL . Based on these results we find a simple model that produces a relatively large non-Gaussianity. We show that t… Show more

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Cited by 22 publications
(74 citation statements)
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“…There is a broad literature on examples and specific realizations of this transfer mechanism from isocurvature to adiabatic perturbations (Bartolo et al 2002;Bernardeau & Uzan 2002;Vernizzi & Wands 2006;Rigopoulos et al 2006Rigopoulos et al , 2007Lyth & Rodriguez 2005;Tzavara & van Tent 2011; for a review on NG from multiple-field inflation models, see Byrnes & Choi 2010). An alternative, important possibility is the curvaton model (Mollerach 1990;Linde & Mukhanov 1997;Enqvist & Sloth 2002;Lyth & Wands 2002;Moroi & Takahashi 2001).…”
Section: Multi-field Modelsmentioning
confidence: 99%
“…There is a broad literature on examples and specific realizations of this transfer mechanism from isocurvature to adiabatic perturbations (Bartolo et al 2002;Bernardeau & Uzan 2002;Vernizzi & Wands 2006;Rigopoulos et al 2006Rigopoulos et al , 2007Lyth & Rodriguez 2005;Tzavara & van Tent 2011; for a review on NG from multiple-field inflation models, see Byrnes & Choi 2010). An alternative, important possibility is the curvaton model (Mollerach 1990;Linde & Mukhanov 1997;Enqvist & Sloth 2002;Lyth & Wands 2002;Moroi & Takahashi 2001).…”
Section: Multi-field Modelsmentioning
confidence: 99%
“…This encompasses, for instance, a large class of multi-field models which leads to non-Gaussian isocurvature perturbations (for earlier works, see e.g., Linde & Mukhanov 1997;Peebles 1997;Bucher & Zhu 1997). More importantly, such models can also lead to cross-correlated and nonGaussian adiabatic and isocurvature modes, where NG is first generated by large nonlinearities in some scalar (possibly noninflatonic) sector of the theory, and then efficiently transferred to the inflaton adiabatic sector(s) through the cross-correlation of adiabatic and isocurvature perturbations 7 (Bartolo et al 2002;Bernardeau & Uzan 2002;Vernizzi & Wands 2006;Rigopoulos et al 2006Rigopoulos et al , 2007Lyth & Rodriguez 2005;Tzavara & van Tent 2011; for a review on NG from multiple-field inflation models, see, Byrnes & Choi 2010). Another interesting possibility is the curvaton model (Mollerach 1990;Enqvist & Sloth 2002;Lyth & Wands 2002;Moroi & Takahashi 2001), where a second light scalar field, subdominant during inflation, decays after inflation ends, producing the primordial density perturbations which can be characterized by a high NG level (e.g., Lyth & Wands 2002;Lyth et al 2003;Bartolo et al 2004d).…”
Section: Multi-field Modelsmentioning
confidence: 99%
“…So the first basis vector is always along the field trajectory as it is defined as the direction of the field velocity. The second basis vector is perpendicular to the first, and since we have only two dimensions it can be completely expressed in terms of the components of the first basis vector (see appendix A of [36] for some refinements of this basis originally introduced in [60]). For later use we will define the following quantities:…”
Section: Background Dynamicsmentioning
confidence: 99%
“…The aims of this paper are threefold. The first is a continuation of the work on the longwavelength formalism, in particular of [36]. In that paper a completely general expression for the f NL produced in two-field inflation on super-Hubble scales was derived.…”
mentioning
confidence: 99%