We study the energy-energy correlator (EEC) in heavy states of four-dimensional super Yang–Mills theory in the large-charge 't Hooft limit, in which the dimension of the heavy operator (or, equivalently, its -charge) is taken to infinity with the effective coupling held fixed. The relevant heavy-heavy-light-light four-point correlators are known to all orders in in this limit. For certain classes of operators, the perturbative series can be resummed to obtain exact finite-coupling expressions. We use these results to determine the corresponding EEC, whose dynamical part can be extracted from a double discontinuity of the four-point correlator. We determine the EEC at finite effective coupling and study its physical behavior as a function of and the angular separation between the detectors, both at generic angles and in the collinear and back-to-back limits.

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