Analytic First-Order Entanglement Entropy of Schwarzschild Black Holes with Interacting Scalars
Florin Manea
TL;DR
This work derives a closed-form first-order correction to the entanglement entropy for a self-interacting scalar field across a Schwarzschild horizon, using the replica trick and heat-kernel methods on a conical manifold. It yields explicit expressions for the correction $δS^{(1)}$ and a renormalized Newton constant $G_F$, revealing a log-enhanced quadratic divergence that is absorbed into the gravitational coupling, leaving a finite Bekenstein–Hawking entropy $S_{BH} = A_{Σ}/(4 G_F)$. The results show how the correction grows with light fields and strong interactions, but is suppressed by curvature and vanishes at leading order for conformally coupled fields ($ξ=1/6$). This analytic framework clarifies the direct link between quantum field interactions, entanglement across horizons, and the renormalization of gravitational couplings within an effective-field-theory interpretation of gravity.
Abstract
We compute the first-order correction to the entanglement entropy of a scalar field with quartic self-interaction across the horizon of a Schwarzschild black hole. The key result is a fully explicit analytic expression for both the renormalized Newton constant and the corresponding correction to the entropy. Using the Euclidean action, the replica trick, and heat-kernel methods, we obtain a closed-form expression that depends directly on the horizon area, the scalar mass, the interaction strength, and the curvature coupling. The correction exhibits a characteristic logarithmically enhanced quadratic divergence, which is absorbed into the renormalized gravitational coupling. Once this renormalization is performed, the entropy takes the standard Bekenstein-Hawking form with a finite, physically meaningful value. Our result makes it possible to study in detail how the correction varies with model parameters: light fields and strong interactions increase the effect, curvature suppresses it, and conformally coupled fields show no leading-order contribution. Overall, this work provides a clear analytic demonstration of how quantum field interactions modify black hole entropy through the renormalization of Newton's constant.
