The primary photochemistry of the blue-light sensor protein, phototropin, is adduct formation between the C4a atom of the flavin mononucleotide (FMN) chromophore and a nearby, reactive cysteine (Cys966), following decay of the triplet excited state of FMN. The distance between the C4a position of FMN and the sulfur atom of Cys966 is 4.2 A in the LOV2 domain of Adiantum neochrome 1 (neo1-LOV2), a fusion protein of phototropin containing the phytochrome chromophoric domain. We previously reported the presence of an unreactive fraction in neo1-LOV2 at low temperatures, which presumably originated from the heterogeneous environment of Cys966 [Iwata, T., Nozaki, D., Tokutomi, S., Kagawa, T., Wada, M., and Kandori, H. (2003) Biochemistry 42, 8183-8191]. The present study showed that (i) 28% forms an adduct at 77 K (state I), (ii) 50% forms an adduct at 150 K but not at 77 K (state II), and (iii) 22% does not form an adduct at 150 K (state III). By Fourier transform infrared (FTIR) spectroscopy, we observed the S-H stretching frequencies at 2570 and 2562 cm-1 for state I and at 2563 cm-1 for state II, suggesting that the microenvironment of the S-H group of Cys966 determines the reactivity at low temperatures. Adduct formation is more efficient for state I than for states II and III. Molecular dynamics simulation strongly suggests that the observed multiple structures originate from the isomeric forms of Cys966. We thus concluded that there are multiple local structures of FMN and cysteine in neo1-LOV2, each of which is thermally converted by protein fluctuation at physiological temperatures.