Nonperturbative structure of lower-degree discrete-volume components

Determine the nonperturbative structure of the lower-degree components of the discrete volumes N_{g,n} governing ETH matrix-model amplitudes, in order to obtain subleading-in-λ corrections beyond those captured by the q-deformed Weil–Petersson volumes V^q_{g,n}.

Background

The leading nonperturbative correction is protected because only the top-degree part of the discrete volume contributes at leading order in the small-λ expansion; this top-degree part is represented by the q-deformed Weil–Petersson volume.

Subleading corrections require the nonperturbative behavior of the lower-degree remainder of N_{g,n}, which the paper does not determine in general. This unresolved input prevents the authors from extending their general method to subleading powers of λ.

References

Section~\ref{sec:N11-N12} already shows what this leaves out: subleading-in-$$ corrections would need the lower-degree remainder's own non-perturbative structure, which is not currently known in general.

The ETH matrix model for DSSYK: non-perturbative corrections and intersection theory  (2608.23298 - Alfinito et al., 24 Aug 2026) in Section 5, From DSSYK discrete volumes to V^q_{g,n}(L)