Genetically encoded non-canonical amino acids reveal asynchronous dark reversion of chromophore, backbone and side-chains in EL222
Photoreceptors containing the light-oxygen-voltage (LOV) domain elicit biological responses upon excitation of their flavin mononucleotide (FMN) chromophore by blue light. The mechanism and kinetics of dark-state recovery are not well understood. Here we incorporated the non-canonical amino acid p-cyanophenylalanine (CNF) by genetic code expansion technology at forty-five positions of the bacterial transcription factor EL222. Screening of light-induced changes in infrared (IR) absorption frequency, electric field and hydration of the nitrile groups identified residues CNF31 and CNF35 as reporters of monomer/oligomer and caged/decaged equilibria, respectively. Time-resolved multi-probe UV/Visible and IR spectroscopy experiments of the lit-to-dark transition revealed four dynamical events. Predominantly, rearrangements around the A helix interface (CNF31 and CNF35) precede FMN-cysteinyl adduct scission, folding of -helices (amide bands), and relaxation of residue CNF151. This study illustrates the importance of characterizing all parts of a protein and suggests a key role for the N-terminal A extension of the LOV domain in controlling EL222 photocycle length. SignificanceThe kinetics of fold switching between non-illuminated and blue-light-irradiated states in the transcription factor EL222 is important for understanding the signal transduction mechanism of LOV photoreceptors. Here we combine two native probes, the FMN chromophore (absorption bands in the UV/Visible region) and the protein backbone (amide bands in the infrared region), with genetically encoded cyano (C{equiv}N)-containing phenylalanine residues as infrared reporters of protein microenvironments. EL222 structural dynamics is more complex than expected if using a single type of probe. Local changes around residues 31 and 35 precede FMN-protein adduct rupture, which in turn precedes the global protein conformational relaxation. Our findings point the way forward to obtaining comprehensive descriptions of kinetic transitions in LOV and other photosensors.