Abstract:We consider inflationary cosmology in the context of string compactifications with multiple throats. In scenarios where the warping differs significantly between throats, string and Kaluza-Klein physics can generate potentially observable corrections to the cosmology of inflation and reheating. First we demonstrate that a very low string scale in the ground state compactification is incompatible with a high Hubble scale during inflation, and we propose that the compactification geometry is altered during infla… Show more
“…Reheating can then induce copious production of excited strings in the strongly warped throat [547]. Analyzing this process in detail remains challenging.…”
Section: Reheatingmentioning
confidence: 99%
“…When the inflationary energy is also localized on a brane, one can take a modular approach, in which the inflationary sector and the visible sector constructed separately, in local geometries approximating regions of some unspecified compactification, and their interactions are then computed or parameterized. This strategy has been fruitful in extensive explorations [545][546][547][548][549][550][551][552][553][554][555][556] in the context of warped D-brane inflation [41], as we review in §5.1. Reheating in other models involving D-branes has been studied in e.g.…”
We review cosmological inflation and its realization in quantum field theory and in string theory. This material is a portion of a book, also entitled Inflation and String Theory, to be published by Cambridge University Press.
“…Reheating can then induce copious production of excited strings in the strongly warped throat [547]. Analyzing this process in detail remains challenging.…”
Section: Reheatingmentioning
confidence: 99%
“…When the inflationary energy is also localized on a brane, one can take a modular approach, in which the inflationary sector and the visible sector constructed separately, in local geometries approximating regions of some unspecified compactification, and their interactions are then computed or parameterized. This strategy has been fruitful in extensive explorations [545][546][547][548][549][550][551][552][553][554][555][556] in the context of warped D-brane inflation [41], as we review in §5.1. Reheating in other models involving D-branes has been studied in e.g.…”
We review cosmological inflation and its realization in quantum field theory and in string theory. This material is a portion of a book, also entitled Inflation and String Theory, to be published by Cambridge University Press.
“…One class of string-theoretic models that has received considerable attention is Dbrane inflation [2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26]. (For recent reviews, see, e.g., [27,28]).…”
Abstract. An upper bound on the amplitude of the primordial gravitational wave spectrum generated during ultra-violet DBI inflation is derived. The bound is insensitive to the form of the inflaton potential and the warp factor of the compactified dimensions and can be expressed entirely in terms of observational parameters once the volume of the five-dimensional sub-manifold of the throat has been specified. For standard type IIB compactification schemes, the bound predicts undetectably small tensor perturbations with a tensor-scalar ratio r < 10 −7 . This is incompatible with a corresponding lower limit of r > 0.1(1 − n s ), which applies to any model that generates a red spectral index n s < 1 and a potentially detectable non-Gaussianity in the curvature perturbation. Possible ways of evading these bounds in more general DBItype scenarios are discussed and a multiple-brane model is investigated as a specific example.
“…Generally we expect a warped space with a very small minimum warp factor to be deformed in the IR side by the Hubble expansion, so the location where the deformation starts to be significant is crucial. So far there have been several kinds of such backreactions discussed in the literature [7,[9][10][11][12]. Particles such as strings can be created in the IR side by the spatial expansion because their mass scales are redshifted.…”
Section: 2)mentioning
confidence: 99%
“…Only when the density of these particles exceeds certain critical value, its backreaction shortens the warped throat; but this still leaves a considerable portion of warped space for DBI inflation [7]. Various moduli that stabilize the IR warp factor in the flux compactification will fluctuate in the inflationary background and this also shortens the throat [9,10]. The analyses along this line so far has not been explicit enough for our purpose due to technical difficulties in solving equations of motion with large warping, and also it is likely to be model-dependent.…”
We show a model-independent fine-tuning issue in the DBI inflationary mechanism. DBI inflation requires a warp factor h small enough to sufficiently slow down the inflaton. On the other hand, the Einstein equation in extra dimensions under the inflationary background deforms the warp space in the IR side. Generically these two locations coincide with each other, spoiling the DBI inflation. The origin and tuning of this "h-problem" is closely related, through the AdS/CFT duality, to those of the well-known "η-problem" in the slowroll inflationary mechanism.
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