Quantifying light–matter interactions is crucial for the design of nanophotonic devices, but remains challenging because excitation, recombination, photon extraction, and collection processes are strongly intertwined. Here, we developed a quantitative framework to decouple these processes by combining angle-resolved photoluminescence (PL), direct PL quantum yield (PLQY), PL lifetime measurements, and full-wave simulations. Our study focuses on large-area one-dimensional photonic crystals (PC) coupled with a thin film of CsPbI3 perovskite nanocrystals (NCs). By intentionally minimizing excitation enhancement through careful system design ( ηexc=1 and ηexc=1.15 for S- and P-polarizations, respectively), we assess emission-side processes as the dominant contributors to the experimentally observed PL enhancement. The system yields a 110‑fold in PL enhancement mediated by quasi-bound states in the continuum (quasi-BIC) while a tenfold enhancement is achieved via normal Bloch resonances, relative to the PL intensity on glass. Our quantitative decomposition reveals that the quasi-BIC enhancement is primarily driven by photon extraction (factor ~21), far exceeding contributions from QY enhancement (factor of 1.94), and collection efficiency (factor of 3.25). In contrast, the enhancement associated with the Bloch resonances (~ tenfold) arise from a more balanced interplay of extraction (factor of 2.71), QY enhancement (1.37) included Purcell-based emission rate enhancement (factor of 1.24), and improved collection efficiency (factor of 3.2). These findings uncover the interplay of concurrent processes and provide a quantitative validation of the reciprocal principle for designing resonant light-emitting surfaces. Our work establishes a broadly applicable framework for evaluating exciton-cavity interactions in lossy systems, enabling precise control of light emission for high-efficiency optoelectronic devices, quantum light sources, and advanced sensing technologies.
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Le et al. (2026) studied this question.
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