2016
DOI: 10.1088/1475-7516/2016/03/006
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Disformally coupled inflation

Abstract: Abstract. A disformal coupling between two scalar fields is considered in the context of cosmological inflation. The coupling introduces novel derivative interactions mixing the kinetic terms of the fields but without introducing superluminal or unstable propagation of the two scalar fluctuation modes. Though the typical effect of the disformal coupling is to inhibit one of the fields from inflating the universe, the energy density of the other field can drive viable near Sitter -inflation in the presence of n… Show more

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Cited by 26 publications
(22 citation statements)
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“…This action encompasses a wide range of models, including coupled and uncoupled two-field models [11,12], those with Diract Born Infeld (DBI) kinetic terms [13], disformally coupled inflation [14], and even many theories with non-standard gravity following a transformation of the action (such as Starobinsky inflation after conformal transformation [15,16]).…”
mentioning
confidence: 99%
“…This action encompasses a wide range of models, including coupled and uncoupled two-field models [11,12], those with Diract Born Infeld (DBI) kinetic terms [13], disformally coupled inflation [14], and even many theories with non-standard gravity following a transformation of the action (such as Starobinsky inflation after conformal transformation [15,16]).…”
mentioning
confidence: 99%
“…These terms appear although the field χ has no contribution to the dynamics of the universe. Hence, these terms could largely alter the oscillation behaviour of the inflaton field during preheating compared with our case, and could modify the feature of inflation compared with that in [26]. However, in this work, we concentrate on the preheating process of model based upon the disformal inflationary scenario investigated in [26], so that we will not consider this situation.…”
Section: Scalar-tensor Theory With the Disformal Couplingmentioning
confidence: 92%
“…(3.26) contain factors of the transfer function T RS , we need a way of computing this. Fortunately, this can be obtained from our numerical simulations of the perturbed equations of motion carried out in section 2 and our previous paper [30], by comparing the final value of P R to its value at horizon-crossing.…”
Section: Non-gaussianitiesmentioning
confidence: 99%