“…Historically, this has involved the enhancement of intersystem crossing (ISC) rates through the design of molecules with singlet–triplet energy level degeneracies − or by incorporating heavy atoms to increase spin–orbit coupling . A related approach involves the incorporation of heteroatoms with low energy nonbonding orbitals, which facilitates fast triplet formation through a process in which a change in spin angular momentum can be offset by a change in orbital angular momentum (El-Sayed rule). , More recently, a strategy for triplet generation in organic molecules has emerged in the form of multichromophore systems capable of singlet fission (SF), which includes a growing list of small molecule chromophores, oligomers, and polymers. − The advantage of SF materials is that a photogenerated singlet exciton rapidly decays into a pair of triplet excitons, allowing for enhanced triplet yields with a quantum yield above 1 on ultrafast time scales. − In optoelectronic applications, the formation of the triplet pair facilitates the utilization of energy that would normally be lost as heat. , Furthermore, it has recently been proposed that photochemical applications may directly benefit from the distinct properties of the triplet pair compared to an individual triplet. , As such, a key challenge is distinguishing between processes that generate an individual triplet versus those that generate a triplet pair. ,, This is necessary to both properly characterize quantum yields and design harvesting interfaces that account for their differing lifetimes and recombination pathways.…”