This randomized trial investigates the renormalized spectral entropy functional's effect on geometric gravity, suggesting implications for effective dynamics.
We investigate the covariant metric variation of a minimal spectral entropy functional \( S_Π[g] = 12 log ' A_g \) defined by a Laplace-type elliptic operator on a four-dimensional Riemannian manifold. Using heat-kernel methods and zeta regularization, we analyze the renormalized functional and determine the geometric structure of the resulting effective stress tensor. We show that the renormalized spectral variation decomposes into a local two-derivative Einstein tensor term, a cosmological term, local four-derivative quadratic curvature contributions, non-local form factors, and a conformal anomaly piece. The Einstein tensor arises from the counterterm associated with the a₂ heat-kernel pole, in direct analogy with induced gravity in the sense of Sakharov. In the weak-curvature regime where all dimensionless curvature invariants satisfy \(R\,ₛₚ^2 1\), the local two-derivative contribution dominates over higher-derivative and non-local terms. The induced Newton coupling scales parametrically with the spectral cutoff as \(G_N ~ 16π^2 ₛₚ^2\), up to scheme-dependent factors. These results show that the infrared-dominant local part of the renormalized spectral entropy variation reproduces the Einstein tensor. We further show that the ultraviolet completion of this infrared sector is uniquely determined, under a coherence extensivity hypothesis, to be of determinantal Born–Infeld type: the action density takes the Eddington-inspired form √-(gμν + ₛₚ²\, Rμν) - √-g. This mechanism does not rely on a specific microscopic completion, but follows from general properties of the renormalized spectral functional. In this sense the resulting Einstein response appears as the universal two-derivative infrared sector of the effective geometric dynamics, and its Born–Infeld completion as the unique admissible spectral ultraviolet extension. Geometric gravity therefore appears as an effective low-energy response of spectral operator structure rather than as a fundamental dynamical input.
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Jérôme Beau (2026) studied this question.
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