Abstract

The α′-complete cosmology developed by Hohm and Zwiebach classifies the O(d, d; ℝ) invariant theories involving metric, b-field and dilaton that only depend on time, to all orders in α′. Some of these theories feature non-perturbative isotropic de Sitter vacua in the string frame, generated by the infinite number of higher-derivatives of O(d, d; ℝ) multiplets. Extending the isotropic ansatz, we construct stable and unstable non-perturbative de Sitter solutions in the string and Einstein frames. The generalized equations of motion admit new solutions, including anisotropic d + 1-dimensional metrics and non-vanishing b-field. In particular, we find dSn+1× Td−n geometries with constant dilaton, and also metrics with bounded scale factors in the spatial dimensions with non-trivial b-field. We discuss the stability and non-perturbative character of the solutions, as well as possible applications.

Highlights

  • A no-go theorem states that there are no stable or unstable dSn solutions for n ≥ 4 at tree-level in heterotic and type II string theories [2], and even further, it is conjectured that no stable or meta-stable dS vacua can exist in a consistent quantum theory of gravity [3,4,5]

  • The α -complete cosmology developed by Hohm and Zwiebach classifies the O(d, d; R) invariant theories involving metric, b-field and dilaton that only depend on time, to all orders in α

  • Understanding the cosmological consequences of classical string theory requires the knowledge of the infinitely many higher order corrections that it induces on the Einstein equations

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Summary

Field variables and action

The seminal framework developed in [6, 7] is based on Sen’s observation [11] that the low energy effective field theory of the universal gravitational sector of string theory in D = d+1 dimensions displays a global O(d, d; R) symmetry to all orders in α , when the fields do not depend on the d spatial coordinates. This symmetry, referred to as ‘duality’, contains the scale-factor duality a ↔ a−1 [16, 17].

Equations of motion including multi-trace corrections
Non-isotropic metric and vanishing b-field
Stability and types of dS solutions
Generalized ansatz of commuting matrices
Equations of motion
Conservation of the Noether charge and b-field dynamics
Generalized non-perturbative dS vacua
Stability of dS solutions
Caveats on non-perturbative dS solutions
Conclusions
A Equations of motion in the generalized ansatz
Diagonalized equations of motion
C Caveats on generalized non-perturbative dS solutions

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