Selective photoexcitation of the donor in an electron donor–acceptor1–acceptor2 (D–A1–A2) molecule, in which D = perylene and both A1 and A2 = naphthalene-1,8:4,5-bis(dicarboximide), results in sub-nanosecond formation of a spin-correlated singlet radical pair 1(D+˙–A1−˙–A2) having a large electron spin–spin exchange interaction, 2J, which precludes its observation by transient EPR spectroscopy. Subsequent selective photoexcitation of A1−˙ rapidly produces 1(D+˙–A1–A2−˙), resulting in a dramatic decrease in 2J, which allows coherent spin evolution to mix the singlet (S) radical pair state 1(D+˙–A1–A2−˙) with the T0 triplet sublevel of 3(D+˙–A1–A2−˙) in an applied magnetic field, where B ≫ 2J. A spin-polarized transient EPR spectrum characteristic of the spin-correlated radical pair D+˙–A1–A2−˙ is then observed. The time delay between the two laser pulses was incremented to measure the rate of decoherence in 1(D+˙–A1−˙–A2) in toluene at 295 K, which was found to be 8.1 × 107 s−1. Deuteration of the perylene donor or the toluene solvent decreases the decoherence rate constant of 1(D+˙–A1−˙–A2) to 4.3 × 107 s−1 and 4.6 × 107 s−1, respectively, while deuteration of both the perylene donor and the toluene solvent reduced the decoherence rate constant by more than half to 3.4 × 107 s−1. The data show that decreasing electron-nuclear hyperfine interactions significantly increases the zero quantum coherence lifetime of the spin-correlated radical pair.