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Solid‐state nuclear magnetic resonance (NMR) is a powerful technique for structure determination with applications ranging from biology to material sciences. However, its inherent low sensitivity prevents many applications. In solids, optical hyperpolarization techniques such as solid‐state photochemically induced dynamic nuclear polarization (photo‐CIDNP) could alleviate this limitation, by generating nuclear spin hyperpolarization. We recently showed that 1 H and 13 C photo‐CIDNP can be observed for synthetic donor–acceptor (D–A) molecules. However, polarization levels in these systems are so far relatively low (