4.4 Article

Cosmological α′-corrections from the functional renormalization group

Journal

JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 6, Pages -

Publisher

SPRINGER
DOI: 10.1007/JHEP06(2021)045

Keywords

Cosmology of Theories beyond the SM; String Duality; Nonperturbative Effects; Renormalization Group

Funding

  1. Scuola Normale Superiore
  2. INFN [IS CSN4-GSS-PI]
  3. Alexander von Humboldt Foundation
  4. Perimeter Institute for Theoretical Physics
  5. Government of Canada through the Department of Innovation, Science and Economic Development Canada
  6. Province of Ontario through the Ministry of Colleges and Universities
  7. Fonds de la Recherche Scientifique FNRS [F.4503.20, T.0022.19]

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In this study, the Functional Renormalization Group techniques were applied in string theory to derive an effective mini-superspace action for cosmological backgrounds in terms of the string scale alpha '. T-duality played a crucial role in classifying perturbative curvature corrections, leading to renormalization group equations with exact solutions in any spacetime dimension D. While an analytic solution with a non-Gaussian ultraviolet fixed point was found around D = 2, no analogous solution was found in D = 4 using polynomial truncations. The study also discussed potential cosmological implications of the findings.
We employ the techniques of the Functional Renormalization Group in string theory, in order to derive an effective mini-superspace action for cosmological backgrounds to all orders in the string scale alpha '. To this end, T-duality plays a crucial role, classifying all perturbative curvature corrections in terms of a single function of the Hubble parameter. The resulting renormalization group equations admit an exact, albeit non-analytic, solution in any spacetime dimension D, which is however incompatible with Einstein gravity at low energies. Within an E-expansion about D = 2, we also find an analytic solution which exhibits a non-Gaussian ultraviolet fixed point with positive Newton coupling, as well as an acceptable low-energy limit. Yet, within polynomial truncations of the full theory space, we find no evidence for an analog of this solution in D = 4. Finally, we comment on potential cosmological implications of our findings.

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