Subleading strong-coupling corrections to higher EEC multipoles

Derive the subleading terms beyond the leading O(1/λ^{s/2}) contributions in the strong-coupling expansion of the energy–energy correlator multipoles c_s(g) in planar SU(N_c) N=4 super-Yang–Mills theory, in particular for c_3 and c_4, by resolving the divergent sums arising from the noncommuting large-λ expansion and summation, and ascertain whether more complicated coupling-dependent terms appear.

Background

Using the detector–source OPE and recent AdS Virasoro–Shapiro amplitude data, the authors obtain leading strong-coupling behavior c_s ∼ λ{-s/2} and new results, including subleading corrections for c_2. For c_3 and c_4, leading terms are determined, but subleading corrections encounter divergent sums when expanding at large λ and then summing over trajectories.

This indicates a noncommutativity of limits and suggests potential appearance of more intricate coupling-dependent structures. Resolving these divergences and computing the subleading terms would complete the strong-coupling picture for higher multipoles and clarify the structure of the expansion.

References

However, the subleading corrections to eq:c3c4 turn out to lead to divergent sums indicating that the large $\lambda$ expansion and the summation do not commute, which is the reason we have been unable to calculate further subleading corrections. This could also indicate appearance of more complicated coupling-dependent terms in the strong-coupling expansion of $c_s$, see e.g.\ .

Conformal collider bootstrap in ${\mathcal N}=4$ SYM  (2512.10796 - Dempsey et al., 11 Dec 2025) in Section 4.2 (Strong-coupling expansion from stringy modes and OPE)