RESUMEN
Single-molecule localization microscopy (SMLM) at cryogenic temperature opens new avenues to investigate intact biological samples at the nanoscale and perform cryo-correlative studies. Genetically encoded fluorescent proteins (FPs) are markers of choice for cryo-SMLM, but their reduced conformational flexibility below the glass-transition temperature hampers efficient cryo-photoswitching. We investigated cryo-switching of rsEGFP2, one of the most efficient reversibly switchable fluorescent proteins at ambient temperature due to facile cis-trans isomerization of the chromophore. UV-visible microspectrophotometry and X-ray crystallography revealed a completely different switching mechanism at â¼110 K. At this cryogenic temperature, on-off photoswitching involves the formation of two off-states in cis conformation with blue-shifted absorption relative to that of the trans protonated chromophore populated at ambient temperature. Only one of these off-states can be switched back to the fluorescent on-state by 405 nm light, while both of them are sensitive to UV light at 355 nm. Superior recovery to the fluorescent on-state by 355 nm light was confirmed at the single-molecule level. This suggests, as also shown by simulations, that employing 355 nm light in cryo-SMLM experiments using rsEGFP2 and possibly other FPs could improve the effective labeling efficiency achievable with this technique. The rsEGFP2 photoswitching mechanism discovered in this work adds to the panoply of known switching mechanisms in fluorescent proteins.
Asunto(s)
Rayos Ultravioleta , Temperatura , Proteínas Luminiscentes/química , Isomerismo , Conformación ProteicaRESUMEN
Combining fluorescence and phosphorescence kinetics, we characterize forward and reverse intersystem crossing (FISC and RISC, respectively) between the singlet and triplet manifolds S â T in photoswitchable (rsEGFP2) and non-photoswitchable (EGFP) green fluorescent proteins upon continuous 488 nm laser excitation at cryogenic temperatures (CTs). Both proteins behave very similarly, with T1 absorption spectra showing a visible peak at 490 nm (10 mM-1 cm-1) and a vibrational progression in the near-infrared (720 to 905 nm). The dark lifetime of T1 is 21-24 ms at 100 K and very weakly temperature-dependent up to 180 K. Above 180 K, T1 lifetimes reduce rapidly to few milliseconds as found at room temperature (RT). FISC and RISC quantum yields are 0.3 and 0.1%, respectively, for both proteins. The light-induced RISC channel becomes faster than the dark reversal at power densities as low as 20 W cm-2. We discuss implications for fluorescence (super resolution-) microscopy at CT and RT.