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One-loop exactness of the cusp partition function in 3d gravity

Establish whether higher-loop quantum corrections to the gravitational partition function on the doubly infinite cusp geometry H^3/(Z × Z) vanish or can be absorbed into a rescaling of the cusp fugacity μ, thereby proving that the cusp partition function is one-loop exact.

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Background

The paper addresses divergences in the AdS3 gravity path integral arising from accumulation points in the spectrum of hyperbolic 3-manifold volumes. The authors propose to renormalize these divergences by including a contribution from the limiting cusped manifold and tuning a fugacity per cusp to cancel the divergence.

A key step in their proposal is the computation of the cusp’s one-loop determinant, which after a modular-invariant regularization yields a contribution proportional to (√τ2 |η(τ)|2){-1}. Using this, they show the cusp can serve as a counterterm matching the divergence found in the modular Poincaré sum over SL(2,ℤ) black holes.

However, the renormalization argument relies on the assumption that the cusp partition function is one-loop exact. The authors explicitly note that higher-loop effects must be checked to validate the exactness or to determine whether they can be absorbed into μ, making this a central unresolved question for the consistency of the proposal.

References

As a next step, one ought to study higher loops. We are assuming that they vanish (or can be absorbed into rescaling μ) but this needs to be checked.

Cusps in 3d gravity (2510.19920 - Stanford et al., 22 Oct 2025) in Section 3.2 (Renormalization of the sum over SL(2,ℤ) black holes), end of subsection