Mechanistic Investigations of Green mEos4b Reveal a Dynamic Long-Lived Dark State.

Green-to-red photoconvertible fluorescent proteins (PCFPs) are key players in advanced microscopy schemes such as photoactivated localization microscopy (PALM). Whereas photoconversion and red-state blinking in PCFPs have been studied intensively, their green-state photophysical behavior has received less attention. Yet dark states in green PCFPs can become strongly populated in PALM schemes and exert an indirect but considerable influence on the quality of data recorded in the red channel. Furthermore, green-state photoswitching in PCFPs can be used directly for PALM and has been engineered to design highly efficient reversibly switchable fluorescent proteins (RSFPs) amenable to various nanoscopy schemes. Here, we demonstrate that green mEos4b efficiently switches to a long-lived dark state through cis-trans isomerization of its chromophore, as do most RSFPs. However, by combining kinetic crystallography, molecular dynamics simulations, and Raman spectroscopy, we find that the dark state in green mEos4b is much more dynamic than that seen in switched-off green IrisFP, a biphotochromic PCFP engineered from the common EosFP parent. Our data suggest that H-bonding patterns maintained by the chromophore in green PCFPs and RSFPs in both their on- and off-states collectively control photoswitching quantum yields. The reduced number of H-bonds maintained by the dynamic dark chromophore in green mEos4b thus largely accounts for the observed lower switching contrast as compared to that of IrisFP. We also compare the long-lived dark states reached from green and red mEos4b, on the basis of their X-ray structures and Raman signatures. Altogether, these data provide a unifying picture of the complex photophysics of PCFPs and RSFPs.

Chromophore twisting in the excited state of a photoswitchable fluorescent protein captured by time-resolved serial femtosecond crystallography.

Chromophores absorb light in photosensitive proteins and thereby initiate fundamental biological processes such as photosynthesis, vision and biofluorescence. An important goal in their understanding is the provision of detailed structural descriptions of the ultrafast photochemical events that they undergo, in particular of the excited states that connect chemistry to biological function. Here we report on the structures of two excited states in the reversibly photoswitchable fluorescent protein rsEGFP2. We populated the states through femtosecond illumination of rsEGFP2 in its non-fluorescent off state and observed their build-up (within less than one picosecond) and decay (on the several picosecond timescale). Using an X-ray free-electron laser, we performed picosecond time-resolved crystallography and show that the hydroxybenzylidene imidazolinone chromophore in one of the excited states assumes a near-canonical twisted configuration halfway between the trans and cis isomers. This is in line with excited-state quantum mechanics/molecular mechanics and classical molecular dynamics simulations. Our new understanding of the structure around the twisted chromophore enabled the design of a mutant that displays a twofold increase in its off-to-on photoswitching quantum yield.

Structural evidence for a two-regime photobleaching mechanism in a reversibly switchable fluorescent protein.

Photobleaching, the irreversible photodestruction of a chromophore, severely limits the use of fluorescent proteins (FPs) in optical microscopy. Yet, the mechanisms that govern photobleaching remain poorly understood. In Reversibly Switchable Fluorescent Proteins (RSFPs), a class of FPs that can be repeatedly photoswitched between nonfluorescent and fluorescent states, photobleaching limits the achievable number of switching cycles, a process known as photofatigue. We investigated the photofatigue mechanisms in the protein IrisFP using combined X-ray crystallography, optical in crystallo spectroscopy, mass spectrometry and modeling approaches. At laser-light intensities typical of conventional wide-field fluorescence microscopy, an oxygen-dependent photobleaching pathway was evidenced. Structural modifications induced by singlet-oxygen production within the chromophore pocket revealed the oxidation of two sulfur-containing residues, Met159 and Cys171, locking the chromophore in a nonfluorescent protonated state. At laser-light intensities typical of localization-based nanoscopy (>0.1 kW/cm(2)), a completely different, oxygen-independent photobleaching pathway was found to take place. The conserved Glu212 underwent decarboxylation concomitantly with an extensive rearrangement of the H-bond network around the chromophore, and an sp(2)-to-sp(3) hybridization change of the carbon atom bridging the chromophore cyclic moieties was observed. This two-regime photobleaching mechanism is likely to be a common feature in RSFPs from Anthozoan species, which typically share high structural and sequence identity with IrisFP. In addition, our results suggest that, when such FPs are used, the illumination conditions employed in localization-based super-resolution microscopy might generate less cytotoxicity than those of standard wide-field microscopy at constant absorbed light-dose. Finally, our data will facilitate the rational design of FPs displaying enhanced photoresistance.

The single T65S mutation generates brighter cyan fluorescent proteins with increased photostability and pH insensitivity.

Cyan fluorescent proteins (CFP) derived from Aequorea victoria GFP, carrying a tryptophan-based chromophore, are widely used as FRET donors in live cell fluorescence imaging experiments. Recently, several CFP variants with near-ultimate photophysical performances were obtained through a mix of site-directed and large scale random mutagenesis. To understand the structural bases of these improvements, we have studied more specifically the consequences of the single-site T65S mutation. We find that all CFP variants carrying the T65S mutation not only display an increased fluorescence quantum yield and a simpler fluorescence emission decay, but also show an improved pH stability and strongly reduced reversible photoswitching reactions. Most prominently, the Cerulean-T65S variant reaches performances nearly equivalent to those of mTurquoise, with QY  = 0.84, an almost pure single exponential fluorescence decay and an outstanding stability in the acid pH range (pK(1/2) = 3.6). From the detailed examination of crystallographic structures of different CFPs and GFPs, we conclude that these improvements stem from a shift in the thermodynamic balance between two well defined configurations of the residue 65 hydroxyl. These two configurations differ in their relative stabilization of a rigid chromophore, as well as in relaying the effects of Glu222 protonation at acid pHs. Our results suggest a simple method to greatly improve numerous FRET reporters used in cell imaging, and bring novel insights into the general structure-photophysics relationships of fluorescent proteins.

Excited State Dynamics of the Green Fluorescent Protein on the Nanosecond Time Scale.

We have introduced a new algorithm in the parallel processing PMEMD module of the AMBER suite that allows MD simulations with a potential involving two coupled torsions. We have used this modified module to study the green fluorescent protein. A coupled torsional potential was adjusted on high accuracy quantum chemical calculations of the anionic chromophore in the first excited state, and several 15-ns-long MD simulations were performed. We have obtained an estimate of the fluorescence lifetime (2.2 ns) to be compared to the experimental value (3 ns), which is, to the best of our knowledge, the first theoretical estimate of that lifetime.

Relation between pH, structure, and absorption spectrum of Cerulean: a study by molecular dynamics and TD DFT calculations.

Molecular dynamics (MD) and quantum mechanical calculations of the Cerulean green fluorescent protein (a variant of enhanced cyan fluorescent protein ECFP) at pH 5.0 and 8.0 are presented, addressing two questions arising from experimental results (Malo et al., Biochemistry 2007;46:9865-9873): the origin of the blue shift of absorption spectrum when the pH is decreased from 8.0 to 5.0, and the lateral chain orientation of the key residue Asp148. We demonstrate that the blue shift is reproduced assuming that a rotation around the single bond of the exocyclic ring of the chromophore takes place when the pH changes from 5.0 to 8.0. We find that Asp148 is protonated and inside the barrel at pH 5.0 in agreement with crystallographic data. However, the hydrogen bond pattern of Asp148 is different in simulations of the solvated protein and in the crystal structure. This difference is explained by a partial closing of the cleft between strands 6 and 7 in MD simulations. This study provides also a structure at pH 8.0: the Asp148 carboxylate group is exposed to the solvent and the chromophore is stabilized in the trans conformation by a tighter hydrogen bond network. This work gives some insight into the relationship between the pH and the chromophore conformation and suggests an interpretation of the very similar fluorescent properties of ECFP and ECFP/H148D. Proteins 2010. (c) 2009 Wiley-Liss, Inc.

Anisotropic united-atoms (AUA) potential for alcohols.

An anisotropic united-atom (AUA4) intermolecular potential has been derived for the family of alkanols by first optimizing a set of charges to reproduce the electrostatic potential of the isolated molecules of methanol and ethanol and then by adjusting the parameters of the OH group to fit selected equilibrium properties. In particular, the proposed potential includes additional extra-atomic charges in order to improve the matching to the electrostatic field. Gibbs ensemble Monte Carlo simulations were performed to determine the phase equilibria, while the critical region was explored by means of grand canonical Monte Carlo simulations combined with histogram reweighting techniques. In order to increase the transferability of the model, only the parameters of the Lennard-Jones OH group have been fitted, the parameters of the other AUA groups are taken from previous works. Nevertheless, a good level of agreement was obtained for all compounds considered in this work. In particular, excellent results were obtained for the Henry constants calculation of different gases in alkanols.

Monitoring protein interactions in the living cell through the fluorescence decays of the cyan fluorescent protein.

Using fluorescence lifetime microspectroscopy and imaging techniques, we have studied the fluorescence of cyan fluorescent protein (CFP) transiently expressed in HEK-293 cells, in the presence or absence of its fluorescence resonance energy transfer (FRET) partner, yellow fluorescent protein (YFP). When the two proteins are attached through a 27-amino-acid linker, a 33 % average efficiency of intramolecular energy transfer is accurately determined inside the cell. Additionally, we observe a systematic quenching of the CFP fluorescence with increasing levels of protein expression. This quenching cannot be accounted for by formation of the previously described dimer of GFP-related proteins, since its magnitude is unchanged when the fluorescent proteins carry the mutation A206K shown to dissociate this dimer in vitro. Even when the intracellular protein concentration largely exceeds the in vitro dissociation constant of the dimer, self-association remains undetectable, either between free proteins or intramolecularly within the CFP-YFP construct. Instead, the detailed concentration effects are satisfactorily accounted for by a model of intermolecular, concentration-dependent energy transfer, arising from molecular proximity and crowding. In the case of CFP alone, we suggest that self-quenching could result from a pseudo-homo FRET mechanism between different, spectrally shifted emissive forms of the protein. These phenomena require careful consideration in intracellular FRET studies.

Cyan fluorescent protein: molecular dynamics, simulations, and electronic absorption spectrum.

The dynamics and electronic absorption spectrum of enhanced cyan fluorescent protein (ECFP), a mutant of green fluorescent protein (GFP), have been studied by means of a 1 ns molecular dynamics (MD) simulation. The two X-ray conformations A' and B' of ECFP were considered. The chromophore was assumed to be neutral, and all titratable residues were taken in their standard protonation state at neutral pH. The protein was embedded in a box of water molecules (and counterions). The first result is that the two conformations A' and B' are found to be stable all along the simulation. Then, an analysis of the hydrogen-bond networks shows strong differences between the two conformations in the surroundings of the nitrogen atom of the indolic part of the chromophore. This is partly due to the imperfection in the beta barrel near the His148 residue, which allows the access of one solvent molecule inside the protein in conformation A'. Finally, quantum mechanical calculations of the electronic transition energies of the chromophore in the charge cloud of the protein and solvent water molecules were performed using the TDDFT method on 160 snapshots extracted every 5 ps of the MD trajectories. It is found that conformations A' and B' exhibit very similar spectra despite different H-bond networks involving the chromophore. This similarity is related to the weak charge transfer involved in the electronic transition and the weak electrostatic field created by ECFP near the chromophore, within the hypotheses made in the present simulation.

Dynamical and structural properties of benzene in supercritical water.

We have employed an anisotropic united atom model of benzene (R. O. Contreras, Ph.D. thesis, Universitat Rovira i Virgili 2002) that reproduces the quadrupolar moment of this molecule through the inclusion of seven point charges. We show that this kind of interaction is required to reproduce the solvation of these molecules in supercritical water. We have computed self-diffusion coefficient and Maxwell-Stefan coefficients as well as the shear viscosity for the mixture water-benzene at supercritical conditions. A strong density and composition dependence of these properties is observed. In addition, our simulations are in qualitative agreement with the experimental evidence that, at medium densities (0.6 g/cm(3) and 673 K), almost half of the benzene molecules have one hydrogen bond with water molecules. We also observe that these bonds are longer lived than the corresponding hydrogen bonds between water molecules. Similarly, we obtain an important reduction of the dielectric constant of the mixture with the increment of the amount of benzene molecules at medium and high densities.