The electronic energy relaxation of 1-nitronaphthalene was studied in nonpolar, aprotic, and protic solvents in the time window from femtoseconds to microseconds. Excitation at 340 or 360 nm populates the Franck–Condon S1(ππ) state, which is proposed to bifurcate into two essentially barrierless nonradiative decay channels with sub-200 fs lifetimes. The first main decay channel connects the S1 state with a receiver Tn state that has considerable nπ character. The receiver Tn state undergoes internal conversion to populate the vibrationally excited T1(ππ) state in 2–4 ps. It is shown that vibrational cooling dynamics in the T1 state depends on the solvent used, with average lifetimes in the range from 6 to 12 ps. Furthermore, solvation dynamics competes effectively with vibrational cooling in the triplet manifold in primary alcohols. The relaxed T1 state undergoes intersystem crossing back to the ground state within a few microseconds in N2-saturated solutions in all the solvents studied. The second minor channel involves conformational relaxation of the bright S1 state (primarily rotation of the NO2-group) to populate a dissociative singlet state with significant charge-transfer character and negligible oscillator strength. This dissociative channel is proposed to be responsible for the observed photochemistry in 1-nitronaphthalene. Ground- and excited-state calculations at the density functional level of theory that include bulk and explicit solvent effects lend support to the proposed mechanism where the fluorescent S1 state decays rapidly and irreversibly to dark excited states. A four-state kinetic model is proposed that satisfactorily explains the origin of the nonradiative electronic relaxation pathways in 1-nitronaphthalene.

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