Generating the curvature perturbation without an inflaton

Generating the curvature perturbation without an inflaton

(February 1, 2008) | David H. Lyth and David Wands
The paper by David H. Lyth and David Wands presents a mechanism for generating the large-scale curvature perturbation in the universe through the late decay of a massive scalar field known as the curvaton. The curvaton acquires a perturbation with an almost scale-invariant spectrum during cosmological inflation, initially as an isocurvature density perturbation. This isocurvature perturbation generates the curvature perturbation after inflation when the curvaton density becomes significant. The isocurvature perturbation disappears if the curvaton decays into thermalized radiation, and any residual isocurvature perturbation is perfectly correlated with the curvature perturbation. The mechanism can also generate curvature perturbations in pre-big bang and ekpyrotic models if the curvaton has a suitable non-canonical kinetic term. The authors discuss the conditions under which this mechanism works, including the oscillation phase of the curvaton field and the decay of the curvaton before neutrino decoupling. They also explore the implications for particle physics models, such as the curvaton being a pseudo-Goldstone boson, and the potential for generating curvature perturbations in pre-big bang and ekpyrotic scenarios. The curvaton mechanism simplifies the requirements for inflation models and allows for a wider range of inflationary theories.The paper by David H. Lyth and David Wands presents a mechanism for generating the large-scale curvature perturbation in the universe through the late decay of a massive scalar field known as the curvaton. The curvaton acquires a perturbation with an almost scale-invariant spectrum during cosmological inflation, initially as an isocurvature density perturbation. This isocurvature perturbation generates the curvature perturbation after inflation when the curvaton density becomes significant. The isocurvature perturbation disappears if the curvaton decays into thermalized radiation, and any residual isocurvature perturbation is perfectly correlated with the curvature perturbation. The mechanism can also generate curvature perturbations in pre-big bang and ekpyrotic models if the curvaton has a suitable non-canonical kinetic term. The authors discuss the conditions under which this mechanism works, including the oscillation phase of the curvaton field and the decay of the curvaton before neutrino decoupling. They also explore the implications for particle physics models, such as the curvaton being a pseudo-Goldstone boson, and the potential for generating curvature perturbations in pre-big bang and ekpyrotic scenarios. The curvaton mechanism simplifies the requirements for inflation models and allows for a wider range of inflationary theories.
Reach us at info@study.space
[slides and audio] Generating the curvature perturbation without an inflaton