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.
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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.\ .