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Slow-Roll Inflation in Non-geometric Flux Compactification

Cesar Damian, Luis R. Diaz-Barron, Oscar Loaiza-Brito, M. Sabido

Abstract

By implementing a genetic algorithm we search for stable vacua in Type IIB non-geometric flux compactification on an isotropic torus with orientifold 3-planes. We find that the number of stable dS and AdS vacua are of the same order. Moreover we find that in all dS vacua the multi-field slow-roll inflationary conditions are fulfilled. Specifically we observe that inflation is driven by the axio-dilaton and the Kähler moduli. We also comment on the existence of one stable dS vacuum in the presence of exotic orientifolds.

Slow-Roll Inflation in Non-geometric Flux Compactification

Abstract

By implementing a genetic algorithm we search for stable vacua in Type IIB non-geometric flux compactification on an isotropic torus with orientifold 3-planes. We find that the number of stable dS and AdS vacua are of the same order. Moreover we find that in all dS vacua the multi-field slow-roll inflationary conditions are fulfilled. Specifically we observe that inflation is driven by the axio-dilaton and the Kähler moduli. We also comment on the existence of one stable dS vacuum in the presence of exotic orientifolds.

Paper Structure

This paper contains 18 sections, 40 equations, 9 figures, 8 tables.

Figures (9)

  • Figure 1: Landscape for non- SUSY vacua with SUSY broken through the complex structure. (a) AdS, (b) dS.
  • Figure 2: Coupling constant versus volume of the internal space for all vacua. De Sitter vacua are marked as $\otimes$ while AdS vacua are marked as $\times$.
  • Figure 3: Landscape for SUSY breaking through all the moduli: (a) AdS vacua, (b) dS vacua
  • Figure 4: Coupling constant versus volume of the internal space.
  • Figure 5: Projections of parameter $\epsilon$ in the plane a) $\psi_2$-$\psi_3$ b) $\psi_2$-$\phi_3$ c) $\phi_2$-$\psi_2$ d) $\phi_2$-$\psi_3$ e) $\phi_2$-$\phi_3$ f) $\phi_3$-$\psi_3$. The rest two real moduli are kept constant at their vev. The red circle denotes the position of the vev's for the two real fields.
  • ...and 4 more figures