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Multi-Natural Inflation in Supergravity

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arxiv 1403.0410 v2 pith:GB5DOVHP submitted 2014-03-03 hep-ph astro-ph.COhep-th

classification hep-phastro-ph.COhep-th
keywords inflationmulti-naturalpossiblehilltopmodelphaserelativesupergravity
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abstract

We show that the recently proposed multi-natural inflation can be realized within the framework of 4D ${\cal N}=1$ supergravity. The inflaton potential mainly consists of two sinusoidal potentials that are comparable in size, but have different periodicity with a possible non-zero relative phase. For a sub-Planckian decay constant, the multi-natural inflation model is reduced to axion hilltop inflation. We show that, taking into account the effect of the relative phase, the spectral index can be increased to give a better fit to the Planck results, with respect to the hilltop quartic inflation. We also consider a possible UV completion based on a string-inspired model. Interestingly, the Hubble parameter during inflation is necessarily smaller than the gravitino mass, avoiding possible moduli destabilization. Reheating processes as well as non-thermal leptogenesis are also discussed.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Schwinger effect in axion inflation on a lattice

    astro-ph.CO 2025-06 unverdicted novelty 7.0 of 10

    Lattice simulations show that Schwinger currents saturate gauge-field production in axion inflation, yielding universal conductivity and magnetic-field values at the onset of strong backreaction.

  2. Stochastic inflation with an extremely large number of $e$-folds

    hep-ph 2019-08 accept novelty 6.0 of 10

    A shallow local minimum added to a hilltop inflation potential can make the typical number of e-folds as large as 10^(10^10), enough for light scalars to reach Bunch-Davies equilibrium.

  3. QCD Axion on Hilltop by a Phase Shift of $\pi$

    hep-ph 2019-08 conditional novelty 5.0 of 10

    A heavy axion inflaton can shift the QCD axion potential by π, placing the QCD axion at the hilltop and allowing f_a ≳ 3×10^9 GeV to explain all dark matter.

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