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Discrete Lorentzian Quantum Gravity

R. Loll

TL;DR

The paper argues that non-perturbative quantum gravity benefits from a Lorentzian, causally structured discretization rather than Euclidean methods, circumventing the problematic Wick rotation in a dynamical spacetime. It introduces Lorentzian dynamical triangulations, with a partition function over causal triangulations and a unique Wick rotation to Euclidean geometries, yielding a distinct universality class and well-defined transfer matrices in low dimensions. In 2d, the model is exactly solvable, featuring a ground-state geometry with $d_H=2$ and robust matter exponents; in 3d, a new intermediate phase exhibits an extended ground-state universe, unlike Euclidean DT where degenerate phases dominate. These results support Lorentzian DT as a promising framework for a non-perturbative theory of quantum gravity, though the 4d case with propagating degrees of freedom remains to be established.

Abstract

Just as for non-abelian gauge theories at strong coupling, discrete lattice methods are a natural tool in the study of non-perturbative quantum gravity. They have to reflect the fact that the geometric degrees of freedom are dynamical, and that therefore also the lattice theory must be formulated in a background-independent way. After summarizing the status quo of discrete covariant lattice models for four-dimensional quantum gravity, I describe a new class of discrete gravity models whose starting point is a path integral over Lorentzian (rather than Euclidean) space-time geometries. A number of interesting and unexpected results that have been obtained for these dynamically triangulated models in two and three dimensions make discrete Lorentzian gravity a promising candidate for a non-trivial theory of quantum gravity.

Discrete Lorentzian Quantum Gravity

TL;DR

The paper argues that non-perturbative quantum gravity benefits from a Lorentzian, causally structured discretization rather than Euclidean methods, circumventing the problematic Wick rotation in a dynamical spacetime. It introduces Lorentzian dynamical triangulations, with a partition function over causal triangulations and a unique Wick rotation to Euclidean geometries, yielding a distinct universality class and well-defined transfer matrices in low dimensions. In 2d, the model is exactly solvable, featuring a ground-state geometry with and robust matter exponents; in 3d, a new intermediate phase exhibits an extended ground-state universe, unlike Euclidean DT where degenerate phases dominate. These results support Lorentzian DT as a promising framework for a non-perturbative theory of quantum gravity, though the 4d case with propagating degrees of freedom remains to be established.

Abstract

Just as for non-abelian gauge theories at strong coupling, discrete lattice methods are a natural tool in the study of non-perturbative quantum gravity. They have to reflect the fact that the geometric degrees of freedom are dynamical, and that therefore also the lattice theory must be formulated in a background-independent way. After summarizing the status quo of discrete covariant lattice models for four-dimensional quantum gravity, I describe a new class of discrete gravity models whose starting point is a path integral over Lorentzian (rather than Euclidean) space-time geometries. A number of interesting and unexpected results that have been obtained for these dynamically triangulated models in two and three dimensions make discrete Lorentzian gravity a promising candidate for a non-trivial theory of quantum gravity.

Paper Structure

This paper contains 16 sections, 16 equations, 11 figures.

Figures (11)

  • Figure 1: At a branching point associated with a spatial topology change, light-cones get "squeezed".
  • Figure 2: Two layers of a 2d Lorentzian triangulation, with spatial slices of constant $t$ and interpolating future-oriented time-like links.
  • Figure 3: A typical 2d Lorentzian space-time, at volume $N_2=18816$ and total proper time $t=168$.
  • Figure 4: The fractal baby-universe structure of 2d Euclidean gravity, artist's impression.
  • Figure 5: A typical Lorentzian geometry in the presence of one Ising model, at volume $N_2=18816$ and total proper time $t=168$.
  • ...and 6 more figures