Effective Spacetime Geometry from Admissible Non-Injective Projection

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Autore principale: Beau, Jérôme
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Lingua:inglese
Pubblicazione: Zenodo 2026
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author Beau, Jérôme
author_facet Beau, Jérôme
contents <div> <p>Continuing from the gauge structure established in the companion paper Q6a, we derive effective spacetime geometry from the admissibility framework of Foundation paper by importing the continuum limit and geometric-extraction theorems of the companion paper Q5b. Under the lifting hypothesis [H-lift] of Q5b and the Mosco hypotheses of Q5a paper, the admissibility filter $\Pi_q$ converges to an effective operator $\mathcal{L}_{\mathrm{eff}}$ on $\mathbb{R}_\tau \times<br>\mathrm{Heis}_3(\mathbb{R})$ whose principal symbol defines a four-dimensional effective metric tensor $g^{\mu\nu}(x) \propto A^{\mu\nu}(x)$ of Lorentzian signature $(-,+,+,+)$ (Q5b Theorems 5.2 and~6.1). In the presence of a localised stationary obstruction to the admissibility flow with spherical symmetry, flux conservation within this effective geometry forces the Schwarzschild metric as the unique stationary exterior solution, with the horizon appearing as a degeneracy of the principal symbol rather than as a singularity of the underlying admissible structure. The Einstein equations emerge as consistency conditions of the emergent geometry, with the Einstein\textendash Hilbert action derived rigorously from the spectral entropy functional in the Gravity paper. The present paper closes the chain $\Pi_q \to \mathcal{L}_{\mathrm{eff}} \to g^{\mu\nu} \to G_{\mu\nu}$. Hypothesis [H-lift], on which the results were originally conditional, has since been proved in Q9; the main geometric results are therefore unconditional with respect to [H-lift]. No dynamical substrate is required at any step.</p> </div>
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id zenodo_https___doi_org_10_5281_zenodo_20100336
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language eng
publishDate 2026
publisher Zenodo
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spellingShingle Effective Spacetime Geometry from Admissible Non-Injective Projection
Beau, Jérôme
Non-injective projection
Emergent spacetime
Admissibility
Effective metric
Lorentzian geometry
Sub-Riemannian geometry
Heisenberg group
Principal symbol
Schwarzschild solution
Einstein equations
Spectral geometry
Induced gravity
<div> <p>Continuing from the gauge structure established in the companion paper Q6a, we derive effective spacetime geometry from the admissibility framework of Foundation paper by importing the continuum limit and geometric-extraction theorems of the companion paper Q5b. Under the lifting hypothesis [H-lift] of Q5b and the Mosco hypotheses of Q5a paper, the admissibility filter $\Pi_q$ converges to an effective operator $\mathcal{L}_{\mathrm{eff}}$ on $\mathbb{R}_\tau \times<br>\mathrm{Heis}_3(\mathbb{R})$ whose principal symbol defines a four-dimensional effective metric tensor $g^{\mu\nu}(x) \propto A^{\mu\nu}(x)$ of Lorentzian signature $(-,+,+,+)$ (Q5b Theorems 5.2 and~6.1). In the presence of a localised stationary obstruction to the admissibility flow with spherical symmetry, flux conservation within this effective geometry forces the Schwarzschild metric as the unique stationary exterior solution, with the horizon appearing as a degeneracy of the principal symbol rather than as a singularity of the underlying admissible structure. The Einstein equations emerge as consistency conditions of the emergent geometry, with the Einstein\textendash Hilbert action derived rigorously from the spectral entropy functional in the Gravity paper. The present paper closes the chain $\Pi_q \to \mathcal{L}_{\mathrm{eff}} \to g^{\mu\nu} \to G_{\mu\nu}$. Hypothesis [H-lift], on which the results were originally conditional, has since been proved in Q9; the main geometric results are therefore unconditional with respect to [H-lift]. No dynamical substrate is required at any step.</p> </div>
title Effective Spacetime Geometry from Admissible Non-Injective Projection
topic Non-injective projection
Emergent spacetime
Admissibility
Effective metric
Lorentzian geometry
Sub-Riemannian geometry
Heisenberg group
Principal symbol
Schwarzschild solution
Einstein equations
Spectral geometry
Induced gravity
url https://doi.org/10.5281/zenodo.20100336