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The effect of strong light-matter coupling on the electronic ground-state energy landscape of a large ensemble of coupled molecules remains an open question, even at the theoretical level, which still suffers from the lack of experimental studies. In the present work, we have conducted a very careful study of the thermodynamic phase equilibrium between the low-spin (LS) and high-spin (HS) states of a molecular spin-crossover (SCO) thin film, strongly coupled to the vacuum field inside a Fabry–Pérot cavity. While the cavity was tuned to be resonant with the intense charge-transfer bands of the SCO complexes in the LS state, allowing a strong-coupling regime to be achieved with a Rabi splitting of up to 670 meV, molecules in the nonabsorbing HS state remain uncoupled to the cavity. Importantly, no significant change in the spin-transition temperature is observed between the LS and HS states under light-matter coupling within the precision limit (1 °C) of our measurements. The present results demonstrate that, although collective strong coupling to electronic excitations can significantly perturb the excited states of molecules, the effect on the ground-state energy levels remains largely negligible (<0.6 meV).
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Hoblos et al. (2025) studied this question.
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