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      Metric perturbations in two-field inflation

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          Abstract

          We study the metric perturbations produced during inflation in models with two scalar fields evolving simultaneously. In particular, we emphasize how the large-scale curvature perturbation \(\zeta\) on fixed energy density hypersurfaces may not be conserved in general for multiple field inflation due to the presence of entropy as well as adiabatic fluctuations. We show that the usual method of solving the linearized perturbation equations is equivalent to the recently proposed analysis of Sasaki and Stewart in terms of the perturbed expansion along neighboring trajectories in field-space. In the case of a separable potential it is possible to compute in the slow-roll approximation the spectrum of density perturbations and gravitational waves at the end of inflation. In general there is an inequality between the ratio of tensor to scalar perturbations and the tilt of the gravitational wave spectrum, which becomes an equality when only adiabatic perturbations are possible and \(\zeta\) is conserved.

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          Most cited references38

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          Constraints on generalized inflationary cosmologies

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            Extended Inflationary Cosmology

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              False Vacuum Inflation with Einstein Gravity

              We investigate chaotic inflation models with two scalar fields, such that one field (the inflaton) rolls while the other is trapped in a false vacuum state. The false vacuum becomes unstable when the inflaton field falls below some critical value, and a first or second order transition to the true vacuum ensues. Particular attention is paid to Linde's second-order `Hybrid Inflation'; with the false vacuum dominating, inflation differs from the usual true vacuum case both in its cosmology and in its relation to particle physics. The spectral index of the adiabatic density perturbation can be very close to 1, or it can be around ten percent higher. The energy scale at the end of inflation can be anywhere between \(10^{16}\)\,GeV and \(10^{11}\)\,GeV, though reheating is prompt so the reheat temperature can't be far below \(10^{11}\,\)GeV. Topological defects are almost inevitably produced at the end of inflation, and if the inflationary energy scale is near its upper limit they can have significant effects. Because false vacuum inflation occurs with the inflaton field far below the Planck scale, it is easier to implement in the context of supergravity than standard chaotic inflation. That the inflaton mass is small compared with the inflationary Hubble parameter is still a problem for generic supergravity theories, but remarkably this can be avoided in a natural way for a class of supergravity models which follow from orbifold compactification of superstrings. This opens up the prospect of a truly realistic, superstring
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                Author and article information

                Journal
                1995-11-08
                Article
                10.1103/PhysRevD.53.5437
                astro-ph/9511029
                3576057e-ed2c-4066-8b4d-7f65a01f4821
                History
                Custom metadata
                SUSSEX-AST-95/11-4, IEM-FT-119/95
                Phys.Rev. D53 (1996) 5437-5445
                RevTex, 9 pages, 1 uuencoded figure appended, also available on WWW via http://star.maps.susx.ac.uk/index.html
                astro-ph gr-qc

                General relativity & Quantum cosmology,General astrophysics
                General relativity & Quantum cosmology, General astrophysics

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