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Non-perturbative summation over 3D discrete topologies

Laurent Freidel, David Louapre

TL;DR

This work addresses how to give a rigorous meaning to summing over all spacetime topologies in 3D quantum gravity by embedding the sum in a group field theory. It introduces modified Boulatov-type GFTs with positive potentials so that their perturbative expansions are uniquely Borel-summable, providing a non-perturbative definition of the full triangulation sum including all topologies. The approach connects familiar 3D gravity amplitudes (Ponzano-Regge) to dynamical triangulations and matrix-model ideas via non-perturbative resummation, and reorganizes generalized triangulations into a controlled real-triangulation framework using pillow interactions. The main contributions are the positivity-driven modification of the GFT potential, the proof of unique Borel summability, and the explicit reinterpretation of the perturbative series as a sum over (regular and irregular) triangulations, offering a concrete path to topology change in quantum gravity. The results open avenues for extending these non-perturbative resummation techniques to higher dimensions and more complex spin-foam models.

Abstract

We construct a group field theory which realizes the sum of gravity amplitudes over all three dimensional topologies trough a perturbative expansion. We prove this theory to be uniquely Borel summable. This shows how to define a non-perturbative summation over triangulations including all topologies in the context of three dimensional discrete gravity.

Non-perturbative summation over 3D discrete topologies

TL;DR

This work addresses how to give a rigorous meaning to summing over all spacetime topologies in 3D quantum gravity by embedding the sum in a group field theory. It introduces modified Boulatov-type GFTs with positive potentials so that their perturbative expansions are uniquely Borel-summable, providing a non-perturbative definition of the full triangulation sum including all topologies. The approach connects familiar 3D gravity amplitudes (Ponzano-Regge) to dynamical triangulations and matrix-model ideas via non-perturbative resummation, and reorganizes generalized triangulations into a controlled real-triangulation framework using pillow interactions. The main contributions are the positivity-driven modification of the GFT potential, the proof of unique Borel summability, and the explicit reinterpretation of the perturbative series as a sum over (regular and irregular) triangulations, offering a concrete path to topology change in quantum gravity. The results open avenues for extending these non-perturbative resummation techniques to higher dimensions and more complex spin-foam models.

Abstract

We construct a group field theory which realizes the sum of gravity amplitudes over all three dimensional topologies trough a perturbative expansion. We prove this theory to be uniquely Borel summable. This shows how to define a non-perturbative summation over triangulations including all topologies in the context of three dimensional discrete gravity.

Paper Structure

This paper contains 14 sections, 1 theorem, 114 equations, 7 figures.

Key Result

Theorem 1

Let $f$ be analytic in the circle $C_R=\{z | \Re(z^{-1}) > R^{-1}\}$ (see figure fig:analyticity) and having an asymptotic expansion with then the asymptotic series is uniquely Borel summable and $f(z)$ can be uniquely reconstructed from it.

Figures (7)

  • Figure 1: Graphical representation of the propagator and potential. The black square stands for the sum over different permutations of the three lines, see (\ref{['eqn:propagator']}).
  • Figure 2: Triangulation generated by the Feynman diagrams
  • Figure 3: Contour for the analytic continuation of $Z(\lambda)$
  • Figure 4: a) Original contour $C$ for defining $D(-\omega)$; b) Deformed contour $C'$to apply the saddle point method.
  • Figure 5: Domain $C_R$ of analyticity for $f$, and the corresponding domain of analyticity for its Borel transform $B_f$, which contains an open neighbourhood of the real positive axis.
  • ...and 2 more figures

Theorems & Definitions (1)

  • Theorem 1: Sokal-Nevalinna