How not to establish the non-renormalizability of gravity
Juliusz Doboszewski, Niels Siegbert Linnemann

TL;DR
This paper critiques the use of the Bekenstein-Hawking entropy formula in arguments about the non-renormalizability of gravity, highlighting issues with semi-classical extrapolations and dimensional reduction scenarios.
Contribution
It challenges the validity of entropy-based arguments against the possibility of a non-perturbatively renormalizable quantum gravity theory.
Findings
Dimensional reduction scenarios can cause Bekenstein-Hawking entropy to diverge.
Semi-classical extrapolations often rely on problematic assumptions.
The entropy argument may not reliably dismiss the renormalizability of gravity.
Abstract
General relativity cannot be formulated as a perturbatively renormalizable quantum field theory. An argument relying on the validity of the Bekenstein-Hawking entropy formula aims at dismissing gravity as non-renormalizable per se, against hopes (underlying programs such as Asymptotic Safety) that d-dimensional GR could turn out to have a non-perturbatively renormalizable d-dimensional quantum field theoretic formulation. In this note we discuss various forms of highly problematic semi-classical extrapolations assumed by both sides of the debate concerning what we call The Entropy Argument, and show that a large class of dimensional reduction scenarios leads to the blow-up of Bekenstein-Hawking entropy.
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