1999
DOI: 10.1016/s0370-2693(99)00602-4
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Perturbations in k-inflation

Abstract: We extend the theory of cosmological perturbations to the case when the "matter" Lagrangian is an arbitrary function of the scalar field and its first derivatives. In particular, this extension provides a unified description of known cases such as the usual scalar field and the hydrodynamical perfect fluid. In addition, it applies to the recently proposed k-inflation, which is driven by non-minimal kinetic terms in the Lagrangian. The spectrum of quantum fluctuations for slow-roll and power law k-inflation is … Show more

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Cited by 1,171 publications
(1,693 citation statements)
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“…One has an attractor point (x 2 s , z 2 s ) = (1.295, 2.522) corresponding to the scaling solution given in Eqs. (35) and (65). In order to ensure the stability of quantum fluctuations, the trajectories are required to be inside the region shown in Fig.…”
Section: Case Of Constant Qmentioning
confidence: 96%
“…One has an attractor point (x 2 s , z 2 s ) = (1.295, 2.522) corresponding to the scaling solution given in Eqs. (35) and (65). In order to ensure the stability of quantum fluctuations, the trajectories are required to be inside the region shown in Fig.…”
Section: Case Of Constant Qmentioning
confidence: 96%
“…An alternative class of models-known as k-inflation [39,237] or P (X) theories [121]-considers the possibility that inflation was driven by non-trivial kinetic effects rather than by a flat potential. An efficient way to model these effects is through the action 84) where P (X, φ) is (so far) an arbitrary function of the inflaton field φ and of its kinetic energy X ≡ − 1 2 (∂φ) 2 .…”
Section: Non-slow-roll: K-inflationmentioning
confidence: 99%
“…In the inflation model, the tensor tilt is generally predicted as n t = −2 [21,22]. The inflation requires a/a = H 2 (1 − ) where =Ḣ/H 2 , and thus −2 < n t < 0.…”
Section: Introductionmentioning
confidence: 99%