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Why do we live in a Riemannian space time ?
General Relativity and Quantum Cosmology · Submitted 29 Oct 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This may explain why low energy gravity is described by a Riemannian connection.
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The abstract, sentence by sentence
We start from the pure Einstein-Hilbert action in Metric Affine Gravity, with the orthonormal metric. We get an effective Levi-Civita Dilaton gravity theory in which the Dilaton field is related to the scaling of the gravitational coupling. When the Weyl symmetry is broken the resulting Einstein-Hilbert term is equivalent to the Levi-Civita one, using the projective invariance of the model, the non-metricity and torsion may be removed, so that we get a theory perfectly equivalent to general relativity. This may explain why low energy gravity is described by a Riemannian connection.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We start from the pure Einstein-Hilbert action in Metric Affine Gravity, with the orthonormal metric. | method 0.88 | 0.59 | 0.03 | asserted 0.86 |
| s1 | We get an effective Levi-Civita Dilaton gravity theory in which the Dilaton field is related to the scaling of the gravitational coupling. | result 0.96 | 0.84 | 0.07 | asserted 1.00 |
| s2 | When the Weyl symmetry is broken the resulting Einstein-Hilbert term is equivalent to the Levi-Civita one, using the projective invariance of the model, the non-metricity and torsion may be removed, so that we get a theory perfectly equivalent to general relativity. | result 0.96 | 0.73 | 0.32 | asserted 0.83 |
| s3 | This may explain why low energy gravity is described by a Riemannian connection. | interpretation 1.00 | 0.39 | 0.87 | hedged possibility 1.00 |
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Original abstract
We start from the pure Einstein-Hilbert action in Metric Affine Gravity, with the orthonormal metric. We get an effective Levi-Civita Dilaton gravity theory in which the Dilaton field is related to the scaling of the gravitational coupling. When the Weyl symmetry is broken the resulting Einstein-Hilbert term is equivalent to the Levi-Civita one, using the projective invariance of the model, the non-metricity and torsion may be removed, so that we get a theory perfectly equivalent to general relativity. This may explain why low energy gravity is described by a Riemannian connection.
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