TY - JOUR
T1 - Fibre inflation
T2 - Observable gravity waves from IIB string compactifications
AU - Cicoli, M.
AU - Burgess, C. P.
AU - Quevedo, F.
PY - 2009
Y1 - 2009
N2 - We introduce a simple string model of inflation, in which the inflaton field can take trans-Planckian values while driving a period of slow-roll inflation. This leads naturally to a realisation of large field inflation, inasmuch as the inflationary epoch is well described by the single-field scalar potential V = V 0(3-4e -(3)1/2). Remarkably, for a broad class of vacua all adjustable parameters enter only through the overall coefficient V 0, and in particular do not enter into the slow-roll parameters. Consequently these are determined purely by the number of e -foldings, N e, and so are not independent: η 2. This implies similar relations among observables like the primordial scalar-to-tensor amplitude, r, and the scalar spectral tilt, n s: r 6(n s-1) 2. N e is itself more model-dependent since it depends partly on the post-inflationary reheat history. In a simple reheating scenario a reheating temperature of T rh 10 9 GeV gives N e 58, corresponding to n s 0.970 and r 0.005, within reach of future observations. The model is an example of a class that arises naturally in the context of type IIB string compactifications with large-volume moduli stabilisation, and takes advantage of the generic existence there of Kähler moduli whose dominant appearance in the scalar potential arises from string loop corrections to the Kähler potential. The inflaton field is a combination of Kähler moduli of a K3-fibered Calabi-Yau manifold. We believe there are likely to be a great number of models in this class - ''high-fibre models'' - in which the inflaton starts off far enough up the fibre to produce observably large primordial gravity waves.
AB - We introduce a simple string model of inflation, in which the inflaton field can take trans-Planckian values while driving a period of slow-roll inflation. This leads naturally to a realisation of large field inflation, inasmuch as the inflationary epoch is well described by the single-field scalar potential V = V 0(3-4e -(3)1/2). Remarkably, for a broad class of vacua all adjustable parameters enter only through the overall coefficient V 0, and in particular do not enter into the slow-roll parameters. Consequently these are determined purely by the number of e -foldings, N e, and so are not independent: η 2. This implies similar relations among observables like the primordial scalar-to-tensor amplitude, r, and the scalar spectral tilt, n s: r 6(n s-1) 2. N e is itself more model-dependent since it depends partly on the post-inflationary reheat history. In a simple reheating scenario a reheating temperature of T rh 10 9 GeV gives N e 58, corresponding to n s 0.970 and r 0.005, within reach of future observations. The model is an example of a class that arises naturally in the context of type IIB string compactifications with large-volume moduli stabilisation, and takes advantage of the generic existence there of Kähler moduli whose dominant appearance in the scalar potential arises from string loop corrections to the Kähler potential. The inflaton field is a combination of Kähler moduli of a K3-fibered Calabi-Yau manifold. We believe there are likely to be a great number of models in this class - ''high-fibre models'' - in which the inflaton starts off far enough up the fibre to produce observably large primordial gravity waves.
KW - Cosmological applications of theories with extra dimensions
KW - Gravity waves / theory
KW - Inflation
KW - String theory and cosmology
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U2 - 10.1088/1475-7516/2009/03/013
DO - 10.1088/1475-7516/2009/03/013
M3 - Article
AN - SCOPUS:65649092974
SN - 1475-7516
VL - 2009
JO - Journal of Cosmology and Astroparticle Physics
JF - Journal of Cosmology and Astroparticle Physics
IS - 3
M1 - 013
ER -