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Finding a unified fluorescence mechanism is essential to develop and utilize fluorescent proteins appropriately. Here, we report the unified role of the 145th residue on the fluorescence efficiency of fluorescent proteins developed from the jellyfish Aequorea victoria by demonstrating the difference and similarity between two representative fluorescent proteins, enhanced green fluorescent protein (eGFP), and enhanced yellow fluorescent protein (eYFP). We determined the fluorescence lifetimes of the 19 different Y145 mutants of eGFP and eYFP by picosecond time-resolved fluorescence spectroscopy. We found that the effect of the 145th mutation on the fluorescence lifetime is significant for eYFP but moderate for eGFP. We compared known crystal structures to clarify the observed difference between eGFP and eYFP. As a result, we conclude that the efficiency of the steric restriction of the chromophore motion by the 145th side chain is essentially the same for both eGFP and eYFP. Meanwhile, the restriction of the chromophore motion by hydrogen bonds is more pronounced for eGFP than for YFP. Balance of the steric effect and hydrogen bonding controls the lifetime of the Y145 mutants for eGFP and eYFP. Furthermore, the steric restriction is induced by the electrostatic effect; the different 145th residue induces a different electrostatic environment around the chromophore. The finding in this study reasonably explains the reported lifetimes of other fluorescent proteins and allows the prediction of the lifetime of unknown fluorescent proteins from jellyfish.

Fluorescent proteins (FPs) are essential tools for advanced microscopy techniques such as super-resolution imaging, single-particle tracking, and quantitative single-molecule counting. Various FPs fused to DNA-binding proteins have been used to observe the subcellular location and movement of specific gene loci in living and fixed bacterial cells. However, quantitative assessments of the properties of FPs for gene locus measurements are still lacking. Here, we assessed various FPs to observe specific gene loci in live and fixed Escherichia coli cells using a fluorescent repressor-operator binding system (FROS), tet operator-Tet repressor proteins (TetR). Tsr-fused FPs were used to assess the intensity and photostability of various FPs (five red FPs: mCherry2, FusionRed, mRFP, mCrimson3, and dKatushka; and seven yellow FPs: SYFP2, Venus, mCitrine, YPet, mClover3, mTopaz, and EYFP) at the single-molecule level in living cells. These FPs were then used for gene locus measurements using FROS. Our results indicate that TetR-mCrimson3 (red) and TetR-EYFP (yellow) had better properties for visualizing gene loci than the other TetR-FPs. Furthermore, fixation procedures affected the clustering of diffusing TetR-FPs and altered the locations of the TetR-FP foci. Fixation with formaldehyde consistently disrupted proper DNA locus observations using TetR-FPs. Notably, the foci measured using TetR-mCrimson3 remained close to their original positions in live cells after glyoxal fixation. This in vivo study provides a cell-imaging guide for the use of FPs for gene-locus observation in E. coli and a scheme for evaluating the use of FPs for other cell-imaging purposes.

Artificial molecular photoswitches that can be reversibly controlled into different configurations by external light stimulation have broad application prospects in various fields, such as materials and chemical biology. Among them, the pyrrole hemithioindigo (PHT) photoswitch has a geometric structure similar to that of the fluorescent protein chromophore. What happens when the chromophore is replaced by PHT, and does it achieve similar functions to the original one? To answer these questions, we carried out ONIOM(QM/MM) and classical molecular dynamics studies on the photoisomerization mechanism and spectroscopic properties of PHT in the fluorescent protein. The results showed that in the protein environment, the fate of excited PHT is governed by the competition between fluorescence emission and hula-twist isomerization. Due to the strong steric hindrance effects caused by the interlacing residues in the protein that restrict the PHT conformation transformation, the cis-to-trans isomerization process of PHT needs to overcome a barrier of at least 4.9 kcal/mol; thus, fluorescence emission is more dominant in competition. It is also found that the intermolecular interaction between LYS67 and the carbonyl oxygen of PHT has a significant effect on the fluorescence emission. These results revealed the photochemical reaction mechanism of a light-driven molecular switch in the fluorescent protein and provided further theoretical support for the field of chemical biology.

Photoswitchable Dronpa (psDronpa) is a unique member of the fluorescent protein family that can undergo reversible photoinduced switching between fluorescent and dark states and has recently been engineered into a dimer (pdDronpaV) that can dissociate and reassociate as part of its photoswitchable pathway. However, the specific details of the protein structure-function relationship of the dimer interface along with how the dimer proteins interact with each other upon chromophore isomerization are not yet clear. Classical molecular dynamics simulations were performed on psDronpa as monomers and dimers as well as the pdDronpaV dimer and with cis / trans chromophore structures. Analysis of the cis and trans isomers of the chromophore illustrated key differences between their interactions with residues in the protein in both the monomer and dimer forms of psDronpa. Examination of the psDronpa dimer showed nonidentical chromophore interactions between the domains, indicating domain directional favoring. Examination of the trans form of pdDronpaV illuminated the importance of hydrogen bonding between the monomeric domains in maintaining their association, as well as illustrating the motion of dissociation of the domains. This discovery offers important information for possible future mutations of pdDronpaV that might be made to accelerate dissociation.

By combining time-resolved fluorescence spectroscopy and molecular biology, we have clearly elucidated the fluorescence mechanism of yellow cameleon YC3.60. YC3.60 is one of the most widely used fundamental calcium ion indicator proteins and is a tandem protein consisting of cyan fluorescent protein, calmodulin, and yellow fluorescent protein. Our results show that the conformational heterogeneity of YC3.60 leads to multiple FRET (fluorescence resonance energy transfer) processes occurring in a variety of structures. In the presence of calcium ions, FRET occurs in 75% of all YC3.60 molecules, and the intramolecular FRET faster than 20 ps is dominant among the three different FRET processes. Even in the absence of calcium ions, FRET occurs in 28% of YC3.60, where intra- and intermolecular FRET with a time constant of 160 ps is dominant among the four different FRET processes. YC3.60 with the immature chromophore, which is 25% of the total, would result in lower contrast on imaging. Conformational heterogeneity arises from the specific association of the two fluorescent proteins. It was clearly shown that the association of fluorescent proteins has a significant impact on the fluorescence mechanism. These observations lead to the promotion of research that elucidates the relationship between the higher-order structure and function of proteins.

Elucidating the origin of large Stokes shift (LSS) in certain fluorescent proteins absorbing in blue/blue-green and emitting in red/far-red has been quite illusive. Using a combination of spectroscopic measurements, corroborated by theoretical calculations, the presence of four distinct forms of the chromophore of the red fluorescent protein mKeima is confirmed, two of which are found to be emissive: a feeble bluish-green fluorescence (∼520 nm), which is enhanced appreciably in a low pH or deuterated medium but significantly at cryogenic temperatures, and a strong emission in red (∼615 nm). Using femtosecond transient absorption spectroscopy, the trans-protonated form is found to isomerize within hundreds of femtoseconds to the cis-protonated form, which further yields the cis-deprotonated form within picoseconds followed by structural reorganization of the local environment of the chromophore. Thus, the mechanism of LSS is substantiated to proceed via stepwise excited-state isomerization followed by proton transfer involving three isomers, leaving the fourth one (trans-deprotonated) as a bystander. The exquisite pH sensitivity of the dual emission is further exploited in fluorescence microscopy.

Single-molecule superresolution microscopy is a powerful tool for the study of biological structures on size scales smaller than the optical diffraction limit. Imaging samples at cryogenic temperatures (77 K) reduces the quantum yield of photobleaching for many fluorescent labels, yielding localization precisions below 10 nm. Cryogenic imaging further enables correlation with cryogenic electron tomography. A key limitation in applying methods such as PALM and STORM to samples maintained at 77 K is the limited number of fluorophores known to undergo efficient turn-on and turn-off mechanisms necessary to control the sparsity of active emitters. We find that mApple, a red-emitting fluorescent protein, undergoes a novel turn-off mechanism in response to simultaneous illumination with two colors of light. This turn-off mechanism enables localization of many individual molecules in initially bright samples, but the final density of localizable emitters is limited by relatively inefficient turn-on (photoactivation). Bulk excitation and emission spectroscopy shows that mApple has access to two distinct emissive states as well as dark states accessible optically or through changes in pH. The bright and stable emission of mApple enables widefield collection of single-molecule emission spectra, which highlight the complex nature and environmental sensitivity of states observed in red fluorescent proteins.

iLOV is an engineered flavin-binding fluorescent protein (FbFP) with applications for in vivo cellular imaging. To expand the range of applications of FbFPs for multicolor imaging and FRET-based biosensing, it is desirable to understand how to modify their absorption and emission wavelengths (i.e., through spectral tuning). There is particular interest in developing FbFPs that absorb and emit light at longer wavelengths, which has proven challenging thus far. Existing spectral tuning strategies that do not involve chemical modification of the flavin cofactor have focused on placing positively charged amino acids near flavin's C4a and N5 atoms. Guided by previously reported electrostatic spectral tunning maps (ESTMs) of the flavin cofactor and by quantum mechanical/molecular mechanical (QM/MM) calculations reported in this work, we suggest an alternative strategy: placing a negatively charged amino acid near flavin's N1 atom. We predict that a single-point mutant, iLOV-Q430E, has a slightly red-shifted absorption and fluorescence maximum wavelength relative to iLOV. To validate our theoretical prediction, we experimentally expressed and purified iLOV-Q430E and measured its spectral properties. We found that the Q430E mutation results in a slight change in absorption and a 4-8 nm red shift in the fluorescence relative to iLOV, in good agreement with the computational predictions. Molecular dynamics simulations showed that the carboxylate side chain of the glutamate in iLOV-Q430E points away from the flavin cofactor, which leads to a future expectation that further red shifting may be achieved by bringing the side chain closer to the cofactor.

The chromophores of reversibly switchable fluorescent proteins (rsFPs) undergo photoisomerization of both the trans and cis forms. Concurrent with cis/trans photoisomerisation, rsFPs typically become protonated on the phenolic oxygen resulting in a blue shift of the absorption. A synthetic rsFP referred to as rsEospa, derived from EosFP family, displays the same spectroscopic behavior as the GFP-like rsFP Dronpa at pH 8.4 and involves the photoconversion between nonfluorescent neutral and fluorescent anionic chromophore states. Millisecond time-resolved synchrotron serial crystallography of rsEospa at pH 8.4 shows that photoisomerization is accompanied by rearrangements of the same three residues as seen in Dronpa. However, at pH 5.5 we observe that the OFF state is identified as the cationic chromophore with additional protonation of the imidazolinone nitrogen which is concurrent with a newly formed hydrogen bond with the Glu212 carboxylate side chain. FTIR spectroscopy resolves the characteristic up-shifted carbonyl stretching frequency at 1713 cm -1 for the cationic species. Electronic spectroscopy furthermore distinguishes the cationic absorption band at 397 nm from the neutral species at pH 8.4 seen at 387 nm. The observation of photoisomerization of the cationic chromophore state demonstrates the conical intersection for the electronic configuration, where previously fluorescence was proposed to be the main decay route for states containing imidazolinone nitrogen protonation. We present the full time-resolved room-temperature X-ray crystallographic, FTIR, and UV/vis assignment and photoconversion modeling of rsEospa.

The development of bright fluorescent proteins (FPs) emitting beyond 600 nm continues to be of interest both from a fundamental perspective in understanding protein-chromophore interactions and from a practical perspective as these FPs would be valuable for cellular imaging. We previously reported ultrafast spectral observations of the excited-state dynamics in mPlum resulting from interconversion between direct hydrogen bonding and water-mediated hydrogen bonding between the chromophore acylimine carbonyl and the Glu16 side chain. Here, we report temperature-dependent steady-state and time-resolved fluorescence measurements of mPlum and its E16H variant, which does not contain a side-chain permitting hydrogen bonding with the acylimine carbonyl. Lowering the temperature of the system freezes interconversion between the hydrogen-bonding states, thus revealing the spectral signatures of the two states. Analysis of the temperature-dependent spectra assuming Boltzmann populations of the two states yields a 205 cm -1 energy difference. This value agrees with the predictions from a quantum mechanics/molecular mechanics study of mPlum (198 cm -1 ). This study demonstrates the first use of cryogenic spectroscopy to quantify the energetics and timescales of FP chromophore structural states that were only previously obtained from computational methods and further confirms the importance of acylimine hydrogen-bonding dynamics to the fluorescence spectral shifts of red FPs.

Fluorescent proteins (FPs) have become ubiquitous tools for biological research and concomitantly they are intriguing molecules that are amenable to study with a wide range of experimental and theoretical tools. This perspective explores the connection between the engineering of improved FPs and basic ideas from physical chemistry that explain their properties and drive the molecular design of brighter and more photostable variants. We highlight some of the progress and the many knowledge gaps in understanding the relationship between FP brightness and photostability. We also explore some of the pertinent remaining questions and suggest ways in which physical chemists might further examine the physical basis of brightness and photostability in these systems.

The unique properties of the photoswitchable protein Dreiklang are attributed to a reversible hydration/dehydration reaction at the imidazolinone ring of the chromophore. Recovery of the fluorescent state, which is associated with a chemical reaction of the chromophore's dehydration, is an important part of the photocycle of this protein. Here we characterize the fluorescent (ON) and nonfluorescent (OFF) states of Dreiklang and simulate the thermal recovery reaction OFF → ON using computational approaches. By using molecular modeling methods including the quantum mechanics/molecular mechanics (QM/MM) technique, we characterize the structures and spectra of the ON- and OFF-states. The results are consistent with available experimental data. The computed reaction profile explains the observed recovery reaction and clarifies the mechanism of chemical transformations in the chromophore-containing pocket in Dreiklang.

Genetically encoded Förster resonance energy transfer (FRET) sensors enable the visualization of ions, molecules, and processes in live cells. However, despite their widespread use, the molecular states that determine sensor performance are usually poorly understood, which limits efforts to improve them. We used dynamic light scattering (DLS) and time-resolved fluorescence anisotropy to uncover the sensing mechanism of ZifCV1.173, a Zn 2+ FRET sensor. We found that the dynamic range (DR) of ZifCV1.173 was dominated by the high FRET efficiency of the Zn 2+ -free state, in which the donor and acceptor fluorescent proteins were closely associated. Mutating the donor-acceptor interface revealed that the DR of ZifCV1.173 could be increased or decreased by promoting or disrupting the donor-acceptor interaction, respectively. Adapting the same mutations to a related sensor showed the same pattern of DR tuning, supporting our sensing mechanism and suggesting that DLS and time-resolved fluorescence anisotropy might be generally useful in the biophysical characterization of other FRET sensors.

Red fluorescent proteins with a large Stokes shift offer a limited autofluorescence background and are used in deep tissue imaging. Here, by introducing the free amino group in Aequorea victoria, the electrostatic charges of the p-hydroxybenzylidene imidazolinone chromophore of green fluorescent protein (GFP) have been altered resulting in an unusual, 85 nm red-shifted fluorescence. The structural and biophysical analysis suggested that the red shift is due to positional shift occupancy of Glu222 and Arg96, resulting in extended conjugation and a relaxed chromophore. Femtosecond transient absorption spectra exhibited that the excited state relaxation dynamics of red-shifted GFP (rGFP) (τ 4 = 234 ps) are faster compared to the A. victoria green fluorescent protein (τ 4 = 3.0 ns). The nanosecond time-resolved emission spectra of rGFP reveal the continuous spectral shift during emission by a solvent reorientation in the chromophore. Finally, the molecular dynamics simulations revealed the rearrangement of the hydrogen bond interactions in the chromophore vicinity, reshaping the symmetric distribution of van der Waals space to fine tune the GFP structure resulting from highly red-shifted rGFP.

Molecular dynamics (MD) simulations were carried out to obtain the conformational changes of the chromophore in the gold fluorescent protein (PDB ID: 1OXF ). To obtain two-photon absorption (TPA) cross-sections, time dependent density functional theory (TD-DFT) computations were performed for chromophore geometries sampled along the trajectory. The TD-DFT computations used the CAM-B3LYP functional and 6-31+G(d) basis set. Results showed that two dihedral angles change remarkably over the simulation time. TPA cross-sections were found to average 13.82 GM for the excitation to S 1 computed from the equilibrium geometries; however, extending the structures with a water molecule and GLU residue, which make H bonds with the chromophore molecule, increased excitation energies and TPA cross-sections significantly. Besides the effects of the surrounding residues and the dihedrals on the spectroscopic properties, some bond lengths affected the excitation energies and the TPA cross-sections significantly (up to ±25-30%), while the effects of the bond angles were smaller (±5%). Overall the present results provide insight into the effects of the conformational flexibility on TPA (with gold fluorescent protein as a specific example) and suggest that further experimental measurements of TPA for the gold fluorescent protein should be undertaken.

The first hyperpolarizability (β) of six fluorescent proteins (FPs), namely, enhanced green fluorescent protein, enhanced yellow fluorescent protein, SHardonnay, ZsYellow, DsRed, and mCherry, has been calculated to unravel the structure-property relationships on their second-order nonlinear optical properties, owing to their potential for multidimensional biomedical imaging. The ONIOM scheme has been employed and several of its refinements have been addressed to incorporate efficiently the effects of the microenvironment on the nonlinear optical responses of the FP chromophore that is embedded in a protective β-barrel protein cage. In the ONIOM scheme, the system is decomposed into several layers (here two) treated at different levels of approximation (method1/method2), from the most elaborated method (method1) for its core (called the high layer) to the most approximate one (method2) for the outer surrounding (called the low layer). We observe that a small high layer can already account for the variations of β as a function of the nature of the FP, provided the low layer is treated at an ab initio level to describe properly the effects of key H-bonds. Then, for semiquantitative reproduction of the experimental values obtained from hyper-Rayleigh scattering experiments, it is necessary to incorporate electron correlation as described at the second-order Møller-Plesset perturbation theory (MP2) level as well as implicit solvent effects accounted for using the polarizable continuum model (PCM). This led us to define the MP2/6-31+G(d):HF/6-31+G(d)/IEFPCM scheme as an efficient ONIOM approach and the MP2/6-31+G(d):HF/6-31G(d)/IEFPCM as a better compromise between accuracy and computational needs. Using these methods, we demonstrate that many parameters play a role on the β response of FPs, including the length of the π-conjugated segment, the variation of the bond length alternation, and the presence of π-stacking interactions. Then, noticing the small diversity of the FP chromophores, these results highlight the key role of the β-barrel and surrounding residues on β, not only because they can locally break the noncentrosymmetry vital to a β response but also because it can impose geometrical constraints on the chromophore.

We characterize computationally a red fluorescent protein (RFP) with the chromophore (Chro) sandwiched between two aromatic tyrosine rings in a triple-decker motif. According to the original proposal [ J. Phys. Chem. Lett. 2013 , 4 , 1743 ], such a tyrosine-chromophore-tyrosine π-stacked construct can be accommodated in the green fluorescent protein (GFP). A recent study [ ACS Chem. Biol. 2016 , 11 , 508 ] attempted to realize the triple-decker motif and obtained an RFP variant called mRojoA-VYGV with two tyrosine residues surrounding the chromophore. The crystal structure showed that only a tyrosine-chromophore pair was involved in π-stacking, whereas the second tyrosine was oriented perpendicularly, edge-to-face with respect to the chromophore. We propose a more promising variant of this RFP with a perfect triple-decker unit achieved by introducing additional mutations in mRojoA-VYGV. The structures and optical properties of model proteins based on the structures of mCherry and mRojoA are characterized computationally by QM(DFT)/MM. The electronic transitions in the protein-bound chromophores are computed by high-level quantum chemical methods. According to our calculations, the triple-decker chromophore unit in the new RFP variant is stable within the protein and its optical bands are red-shifted with respect to the parent mCherry and mRojoA species.

We report on novel variants of the flavin-based fluorescent protein iLOV with absorption and emission optical bands shifted to the longer wavelengths relative to their precursor. First attempts (J. Phys. Chem. B 2015, 119, 5176; 2016, 120, 3344) to improve spectral properties of iLOV, a fluorescent marker in living cells, showed that single point mutation Q489K could lead to a promising variant, but its realization was not successful due to unfavorable conformation of the flexible lysine side chain pointing away from the chromophore. The results of molecular simulations presented in this work evidence that location of the charged lysine residue near the chromophore isoalloxazine ring can be fixed by introducing additional mutations in iLOV. Several suggested protein variants are characterized by using classical and QM/MM molecular dynamics simulations followed by optimization of structures in the ground and excited states. Transition energies between the S 0 and S 1 states are computed by using the advanced quantum chemical methods TD-DFT, SOS-CIS(D), and XMCQDPT2. According to our simulations, the chromophore-containing pockets for the red-shifted iLOV variants containing lysine either at position 392 (V392K/F410V/A426S) or at position 489 (Q489K/L470T) should be stable and exhibit absorption and emission bands red-shifted by 40-50 nm relative to iLOV.

Living cells are crowded with macromolecules and organelles. As a result, there is an urgent need for molecular sensors for quantitative, site-specific assessment of the macromolecular crowding effects on a myriad of biochemical processes toward quantitative cell biology and biophysics. Here we investigate the excited-state dynamics and translational diffusion of a novel FRET sensor (mCerulean-linker-mCitrine) in a buffer (PBS, pH 7.4) at room temperature. Complementary experiments were carried out on free CFP, YFP, and the cleaved FRET probe as controls. The wavelength-dependent fluorescence lifetime measurements of the donor and acceptor in the FRET probe, using the time-correlated single-photon counting technique, indicate an energy transfer efficiency of 6.8 ± 0.9% in PBS, with distinct excited-state dynamics from the recombinant CFP and YFP. The estimated mCerulean-mCitrine distance in this FRET probe is 7.7 ± 0.2 nm. The energy transfer efficiency increases (11.5 ± 0.9%) as the concentration of Ficoll-70 increases over the range of 0-300 g/L with an estimated mCerulean-mCitrine distance of 6.1 ± 0.2 nm. Complementary time-resolved anisotropy measurements suggest that the rotational diffusion of hetero-FRET in PBS is sensitive to the energy transfer from the donor to the acceptor. The results also suggest that the linker, -(GSG) 6 A(EAAAK) 6 A(GSG) 6 A(EAAAK) 6 A(GSG) 6 -, is rather flexible, and the observed rotational dynamics is likely to be due to a segmental mobility of the FRET pairs rather than an overall tumbling motion of a rigid probe. Comparative studies on a new construct of a FRET probe with a shorter, more flexible linker, mCerulean-(GSG) 18 -mCitrine, reveal enhanced energy transfer efficiency. On the millisecond time scale, fluorescence fluctuation analyses of the acceptor (excited at 488 nm) provide a means to examine the translational diffusion coefficient of the FRET probe. The results also suggest that the linker is flexible in this FRET probe, and the observed diffusion coefficient is faster than predicted as compared to the cleaved FRET probe. Our results serve as a point of reference for this FRET probe in a buffer toward its full potential as a sensor for macromolecular crowding in living cells and tissues.

The search for biocompatible ionic liquids (ILs) with novel biochemical and biomedical applications has recently gained greater attention. In this report, we characterize the effects of two novel amino acid-based aqueous ILs composed of tetramethylguanidinium (TMG) and amino acids on the structure and stability of a widely used red fluorescent protein (mCherry). Our experimental data shows that while the aspartic acid-based IL (TMGAsp) has effects similar to previously studied conventional ILs (BMIBF 4 , EMIAc, and TMGAc), the alanine-based IL (TMGAla) has a much stronger destabilization effect on the protein structure. Addition of 0.30 M TMGAla to mCherry decreases the unfolding temperature from 83 to 60 °C. Even at 25 °C, TMGAla results in a blue shift of the mCherry absorbance and fluorescence peaks and an increased Stokes shift. Molecular dynamics simulations show that the chromophore conformation and its interaction with mCherry with TMGAla are changed relative to those with TMGAsp or in the absence of ILs. Protein-ILs contact analysis indicates that the mCherry-Asp interactions are hydrophilic but the (fewer) mCherry-Ala interactions are more hydrophobic and may modulate the TMG interaction with the protein. Hence, the anion hydrophobicity may explain the special TMGAla destabilization of mCherry.

The yellow fluorescent protein (YFP) is frequently used in a protein complementation assay called bimolecular fluorescence complementation (BiFC), and is employed to visualize protein-protein interactions. In this analysis, two different, nonfluorescent fragments of YFP are genetically attached to proteins of interest. Upon interaction of these proteins, the YFP fragments are brought into proximity close enough to reconstitute their original structure, enabling fluorescence. BiFC allows for a straightforward readout of protein-protein interactions and furthermore facilitates their functional investigation by in vivo imaging. Furthermore, it has been observed that the available color range in BiFC can be extended upon complementing fragments of different proteins that are, like YFP, derived from the Aequorea victoria green fluorescent protein, thereby allowing for a multiplexed investigation of protein-protein interactions. Some spectral characteristics of "multicolor" BiFC (mcBiFC) complexes have been reported before; however, no in-depth analysis has been performed yet. Therefore, little is known about the photophysical characteristics of these mcBiFC complexes because a proper characterization essentially relies on in vitro data. This is particularly difficult for fragments of autofluorescent proteins (AFPs) because they show a very strong tendency to form supramolecular aggregates which precipitate ex vivo. In this study, this intrinsic difficulty is overcome by directly fusing the coding DNA of different AFP fragments. Translation of the genetic sequence in Escherichia coli leads to fully functional, highly soluble fluorescent proteins with distinct properties. On the basis of their construction, they are designated chimeric AFPs, or BiFC chimeras, here. Comparison of their spectral characteristics with experimental in vivo BiFC data confirmed the utility of the chimeric proteins as a BiFC model system. In this study, nine different chimeras were thoroughly analyzed at both the ensemble and the single-molecular level. The data indicates that mutations believed to be photophysically silent significantly alter the properties of AFPs.

By applying molecular dynamics (MD) simulations and quantum chemical calculations, we have characterized the states and processes involved in the excited-state proton transfer (ESPT) of LSSmKate1. MD simulations identify two stable structures in the electronic ground state of LSSmKate1, one with a protonated chromophore and the other with a deprotonated chromophore, thus leading to two separate low-energy absorption maxima with a large energy spacing, as observed in the calculated and experimentally measured absorption spectra. Proton transfer is induced by electronic excitation. When LSSmKate1 is excited, the electrons in the chromophore are transferred from the phenol ring to the N-acylimine moiety; the acidity of a phenolic hydroxyl group is thus enhanced. The calculated potential energy curves (PECs) exhibit energetic feasibility in the generation of the fluorescent species in LSSmKate1, and the exact agreement between the calculated and experimentally measured values of the large Stokes shift further provides solid theoretical evidence for the ESPT process taking place in photoexcited LSSmKate1. The molecular environments play a significant role in the geometries and absorption/emission energies of the chromophores. Overall, TD-ωB97X-D/molecular mechanics (MM) provides a better description of the optical properties of LSSmKate1 than TD-B3LYP/MM, although it always overestimates the excitation energies.

The effective fragment potential (EFP) approach, which can be described as a nonempirical polarizable force field, affords an accurate first-principles treatment of noncovalent interactions in extended systems. EFP can also describe the effect of the environment on the electronic properties (e.g., electronic excitation energies and ionization and electron-attachment energies) of a subsystem via the QM/EFP (quantum mechanics/EFP) polarizable embedding scheme. The original formulation of the method assumes that the system can be separated, without breaking covalent bonds, into closed-shell fragments, such as solvent and solute molecules. Here, we present an extension of the EFP method to macromolecules (mEFP). Several schemes for breaking a large molecule into small fragments described by EFP are presented and benchmarked. We focus on the electronic properties of molecules embedded into a protein environment and consider ionization, electron-attachment, and excitation energies (single-point calculations only). The model systems include chromophores of green and red fluorescent proteins surrounded by several nearby amino acid residues and phenolate bound to the T4 lysozyme. All mEFP schemes show robust performance and accurately reproduce the reference full QM calculations. For further applications of mEFP, we recommend either the scheme in which the peptide is cut along the Cα-C bond, giving rise to one fragment per amino acid, or the scheme with two cuts per amino acid, along the Cα-C and Cα-N bonds. While using these fragmentation schemes, the errors in solvatochromic shifts in electronic energy differences (excitation, ionization, electron detachment, or electron-attachment) do not exceed 0.1 eV. The largest error of QM/mEFP against QM/EFP (no fragmentation of the EFP part) is 0.06 eV (in most cases, the errors are 0.01-0.02 eV). The errors in the QM/molecular mechanics calculations with standard point charges can be as large as 0.3 eV.

Light, oxygen, voltage (LOV) based fluorescent proteins (FPs) represent a promising alternative to fluorescent reporters of the green fluorescent protein family. For certain applications like multicolor imaging or the design of FRET-based biosensors, the generation of spectrally shifted LOV-based FPs would be required. In a recent theoretical study ( Khrenova J. Phys. Chem. B 2015 , 119 ( 16 ), pp 5176 - 5183 ), the photophysical properties of a variant of the LOV-based fluorescent protein iLOV were predicted using quantum mechanics/molecular mechanics (QM/MM) approaches. The variant contained a lysine residue at the position of a highly conserved glutamine residue (Q489K), which directly interacts with the O4 and N5 atom of the flavin mononucleotide (FMN) chromophore. On the basis of QM/MM calculations, iLOV-Q489K was suggested to possess substantially red-shifted absorption and fluorescence-emission maxima with respect to parental iLOV. Here, we describe the experimental characterization of this variant, which, surprisingly contrary to the theoretical prediction, shows blue-shifted absorption and fluorescence-emission maxima. Using molecular dynamics (MD) simulations and QM/MM calculations, the molecular basis for the contradictory theoretical and experimental results is presented. Essentially, our computational analysis suggests that, in the Q489K variant, two possible side-chain conformers exist: (i) a least populated conformer K489in forming a hydrogen bond with the O4 atom of FMN chromophore and (ii) a most populated conformer K489out with the side-chain amino group flipped away from the FMN chromophore forming a new hydrogen bond with the backbone oxygen of G487. QM/MM calculated spectra of the K489out conformer are blue-shifted compared to the calculated spectra of parental iLOV, which is in accordance with experimental data. This suggests that the change in the conformation of K489 from K498in to K489out accounts for the change in the direction of the spectral shift from red to blue, thus reconciling theory and experiment.

Dronpa is a novel photochromic fluorescent protein that exhibits fast response to light. The present article is the first report of the resonance and preresonance Raman spectra of Dronpa. We used the intensity and frequency of Raman bands to determine the structure of the Dronpa chromophore in two thermally stable photochromic states. The acid-base equilibrium in one photochromic state was observed by spectroscopic pH titration. The Raman spectra revealed that the chromophore in this state shows a protonation/deprotonation transition with a pKa of 5.2 ± 0.3 and maintains the cis configuration. The observed resonance Raman bands showed that the other photochromic state of the chromophore is in a trans configuration. The results demonstrate that Raman bands selectively enhanced for the chromophore yield valuable information on the molecular structure of the chromophore in photochromic fluorescent proteins after careful elimination of the fluorescence background.

It is frequently assumed that fluorescent protein tags used in biological imaging experiments are minimally perturbing to their host protein. As in-cell experiments become more quantitative and measure rates and equilibrium constants, rather than just "on-off" activity or the presence of a protein, it becomes more important to understand such perturbations. One criterion for a protein modification to be a perturbation is additivity of two perturbations (a linear effect on the protein free energy). Here we show that adding fluorescent protein tags to a host protein in vitro has a large nonadditive effect on its folding free energy. We compare an unlabeled, three singly labeled, and a doubly labeled enzyme (phosphoglycerate kinase). We propose two mechanisms for nonadditivity. In the "quinary interaction" mechanism, two tags interact transiently with one another, relieving the host protein from unfavorable tag-protein interactions. In the "crowding" mechanism, adding two tags provides the minimal crowding necessary to overcome destabilizing interactions of individual tags with the host protein. Both of these mechanisms affect protein stability in cells; we show here that they must also be considered for tagged proteins used for reference in vitro.

Polymer conjugation for protein-based therapeutics has been developed extensively, but it still suffers from conjugation leading to decrease in protein activity and generates complexes with limited diversity due to general classical systems only incorporating one protein per each complex. Here we introduce a site-specific noncovalent protein-polymer conjugation, which can reduce the heterogeneity of the conjugates without disrupting protein function, while allowing for the modulation of binding affinity and stability, affecting the pH dependent binding of the number of proteins per polymer. We compared classical one protein-polymer conjugates with multiple protein-polymer conjugates using His-tagged enhanced yellow fluorescence protein (His6-eYFP) and metal-coordinated tris-nitrilotriacetic acid (trisNTA-Me(n+)) in a site-specific way. trisNTA-Me(n+)-His6 acts as a reversible linker with pH-triggered release of functional protein from the trisNTA-functionalized copolymers. The nature of the selected Me(n+) and number of available trisNTA-Me(n+) on poly(N-isopropylacrylamide-co-tris-nitrilotriacetic acid acrylamide) (PNTn) copolymers enables predictable modulation of the conjugates binding affinity (0.09-1.35 μM), stability, cell toxicity, and pH responsiveness. This represents a promising platform that allows direct control over the properties of multiple protein-polymer conjugates compared to the classical single protein-polymer conjugates.

The reversible photoswitching of the photochromic fluorescent protein Padron0.9 involves a cis-trans isomerization of the chromophore. Both isomers are subjected to a protonation equilibrium between a neutral and a deprotonated form. The observed pH dependent absorption spectra require at least two protonating groups in the chromophore environment modulating its proton affinity. Using femtosecond transient absorption spectroscopy, we elucidate the primary reaction steps of selectively excited chromophore species. Employing kinetic and spectral modeling of the time dependent transients, we identify intermediate states and their spectra. Excitation of the deprotonated trans species is followed by excited state relaxation and internal conversion to a hot ground state on a time scale of 1.1-6.5 ps. As the switching yield is very low (Φtrans→cis = 0.0003 ± 0.0001), direct formation of the cis isomer in the time-resolved experiment is not observed. The reverse switching route involves excitation of the neutral cis chromophore. A strong H/D isotope effect reveals the initial reaction step to be an excited state proton transfer with a rate constant of kH = (1.7 ps)(-1) (kD = (8.6 ps)(-1)) competing with internal conversion (kic = (4.5 ps)(-1)). The deprotonated excited cis intermediate relaxes to the well-known long-lived fluorescent species (kr = (24 ps)(-1)). The switching quantum yield is determined to be low as well, Φcis→trans = 0.02 ± 0.01. Excitation of both the neutral and deprotonated cis chromophores is followed by a ground state proton transfer reaction partially re-establishing the disturbed ground state equilibrium within 1.6 ps (deuterated species: 5.6 ps). The incomplete equilibration reveals an inhomogeneous population of deprotonated cis species which equilibrate on different time scales.

The iLOV protein is one of the most promising members of the family of engineered flavin-based fluorescent proteins (FbFPs), considered as an alternative to the green fluorescent protein family. We modeled the spectral properties of iLOV using quantum chemistry, quantum mechanics/molecular mechanics (QM/MM), and molecular dynamics approaches. Computational results predict that the conserved Gln489 side chain in iLOV adopts two almost equally populated conformations, Glnin and Glnout, altering hydrogen bonding near the flavin chromophore. Formation of the flavinN5-Gln489 and flavinO4-Gln489 hydrogen bonds in the case of Glnin accounts for the pronounced shifts of the flavin absorption and fluorescence maxima to the longer wavelengths. Following these results, we propose to introduce a point mutation in iLOV, Q489K, with the aim to obtain a more red-shifted variant. According to our simulations, this mutation should lead to a considerable, about 50 nm, red shift of the absorption and emission band maxima, thus introducing a new color in the FbFP palette.

The field of bioimaging and biosensors has been revolutionized by the discovery of fluorescent proteins (FPs) and their use in live cells. FPs are characterized with rich photodynamics due to the presence of nonfluorescent or dark states which are responsible for fluorescence intermittency or "blinking", which has been exploited in several localization-based super-resolution techniques that surpass the diffraction-limited resolution of conventional microscopy. Molecules that convert to these dark states recover to the ground states either spontaneously or upon absorption of another photon, depending on the particular FP and the structural transition that is involved. In this work, we demonstrate time- and frequency-domain methods for the measurement of the ground-state recovery (GSR) times of FPs both in live cells and in solutions. In the time-domain method, we excited the sample with millisecond pulses at varying dark times to obtain percent-recovery. In the frequency-domain method, dark-state hysteresis was employed to obtain the positive phase shift or "phase advance". We extracted the GSR time constants from our measurements using calculations and simulations based on a three-state model system. The GSR time constants of the red FPs studied in these experiments fall in the range from μs to msec time-scales. We find that the time- and frequency-domain techniques are complementary to each other. While accurate GSR times can be extracted from the time-domain technique, frequency-domain measurements are primarily sensitive to the rates of dark-state conversion (DSC) processes. A correlation between GSR times, DSC, and photobleaching rates for the red FPs mCherry, TagRFP-T, and Kriek were observed. These time- and frequency-domain methods can be used in high-throughput screening and sorting of FPs clones based on GSR time constant and photostability and will therefore be valuable for the development of new photoswitchable or photoactivatable FPs.

The electronic circular dichroism (ECD) properties of the green fluorescent protein and other fluorescent proteins have been calculated with density functional theory. The influence of different embedding models on the ECD signal of the chromophore has been investigated by modeling the protein environment by the polarizable continuum model (QM/PCM), by the polarizable embedding model (PE-QM/MM), by treating the minimal environment quantum mechanically at the same footing as the chromophore (QM/QM), and by adding the remaining part of the protein by means of PCM (QM/QM/PCM). The rotatory strength is found to be more sensitive than the oscillatory strength to changes in the geometry of the chromophore and its surroundings and to the type of embedding model used. In general, explicit embedding of the surrounding protein (PE-QM/MM or QM/QM) induces an increase in the rotatory strength of the chromophore. Explicit inclusion of the whole protein through polarizable embedding is found to be an affordable embedding model that gives the correct sign of the rotatory strength for all fluorescent proteins. PCM is useful as a first approximation to protein environment effects, but as a rule seems to underestimate the rotatory strength.

Red fluorescent proteins (RFPs) are widely used probes for monitoring subcellular processes with extremely high spatial and temporal precision. In this work, we employed spectrally resolved transient absorption (SRTA) and two-dimensional double quantum coherence (2D2Q) spectroscopy to investigate the excited state electronic structure of mPlum, a well-known RFP. The SRTA spectra reveal the presence of excited state absorption features at both the low- and high-energy sides of the dominant ground state bleach contribution. The 2D2Q spectra measured at several excitation wavelengths reveal a peak pattern consistent with the presence of more than three electronic states (i.e., ground, excited, and doubly excited). Numerical modeling of this response suggests that the features are consistent with a 1-1-2 electronic structure. The two closely spaced (∼1500 cm(-1)) levels in the double quantum manifold appear at opposite anharmonicities relative to twice the energy of the lowest energy transition. These observations explain the excited state absorption contributions observed in spectrally resolved transient grating and transient absorption measurements and demonstrate the utility of multidimensional spectroscopy in unraveling congested spectra relative to conventional one-dimensional methods.

The fast-switching M159T mutant of the reversibly photoswitchable fluorescent protein Dronpa has an enhanced yield for the on-to-off reaction. The forward and reverse photoreactions proceed via cis-trans and trans-cis photoisomerization, yet protonation and deprotonation of the hydroxyphenyl oxygen of the chromophore is responsible for the majority of the resulting spectroscopic contrast. Ultrafast visible-pump, infrared-probe spectroscopy was used to detect the picosecond, nanosecond, as well as metastable millisecond intermediates. Additionally, static FTIR difference measurements of the Dronpa-M159T mutant correspond very closely to those of the wild type Dronpa, identifying the p-hydroxybenzylidene-imidazolinone chromophore in the cis anion and trans neutral forms in the bright "on" and dark "off" states, respectively. Green excitation of the on state is followed by dominant radiative decay with characteristic time constants of 1.9 ps, 185 ps, and 1.1 ns, and additionally reveals spectral changes belonging to the species decaying with a 1.1 ns time constant, associated with both protein and chromophore modes. A 1 ms measurement of the on state identifies bleach features that correspond to those seen in the static off-minus-on Fourier transform infrared (FTIR) difference spectrum, indicating that thermal protonation of the hydroxyphenyl oxygen proceeds within this time window. Blue excitation of the off state directly resolves the formation of the primary photoproduct with 0.6 and 14 ps time constants, which is stable on the nanosecond time scale. Assignment of the primary photoproduct to the cis neutral chromophore in the electronic ground state is supported by the frequency positions expected relative to those for the nonplanar distorted geometry for the off state. A 1 ms measurement of the off state corresponds closely with the on-minus-off FTIR difference spectrum, indicating thermal deprotonation and rearrangement of the Arg66 side chain to be complete.

Kindling fluorescent protein (KFP), one of the chronologically first members of photoswitchable colored proteins from the green fluorescent protein (GFP) family, increasingly attracts efforts from experimental and theoretical sides. Ambiguous conclusions in solving puzzles of photochemistry of KFP and of its parent natural protein asFP595 are partially explained by lack of reliable theoretical data on chromophore properties in the electronically excited state. We report the results of state-of-the-art quantum chemistry calculations of the structure and energy of the KFP chromophore, 2-acetyl-,4-(p-hydroxybenzylidene)-1-methyl-5-imidazolone (AHBMI), both in the ground and excited states. Ground state equilibrium structures of anionic and zwitterionic protonation states of AHBMI were computed by the conventional MP2 method while excited state structures were characterized by the extended multireference perturbation theory method XMCQDPT2 including optimization of geometry parameters at this level. In particular, the computational results demonstrate that the basicity of the N2 nitrogen atom of the imidazolinone ring should noticeably increase upon electronic excitation, thus affecting excited state proton transfer events in proteins. The results of these simulations as well as of quantum mechanical-molecular mechanical (QM/MM) calculations for model protein systems evidence that KFP conformations with the zwitterionic chromophore are hardly expected to occur in the ground state, but may be populated upon excitation.

Genetically encoded fluorescent proteins (FPs), and biosensors based on them, provide new insights into how living cells and tissues function. Ultimately, the goal of the bioimaging community is to use these probes deep in tissues and even in entire organisms, and this will require two-photon laser scanning microscopy (TPLSM), with its greater tissue penetration, lower autofluorescence background, and minimum photodamage in the out-of-focus volume. However, the extremely high instantaneous light intensities of femtosecond pulses in the focal volume dramatically increase the probability of further stepwise resonant photon absorption, leading to highly excited, ionizable and reactive states, often resulting in fast bleaching of fluorescent proteins in TPLSM. Here, we show that the femtosecond multiphoton excitation of red FPs (DsRed2 and mFruits), both in solution and live cells, results in a chain of consecutive, partially reversible reactions, with individual rates driven by a high-order (3-5 photon) absorption. The first step of this process corresponds to a three- (DsRed2) or four-photon (mFruits) induced fast isomerization of the chromophore, yielding intermediate fluorescent forms, which then subsequently transform into nonfluorescent products. Our experimental data and model calculations are consistent with a mechanism in which ultrafast electron transfer from the chromophore to a neighboring positively charged amino acid residue triggers the first step of multiphoton chromophore transformations in DsRed2 and mFruits, consisting of decarboxylation of a nearby deprotonated glutamic acid residue.

Red fluorescent proteins (RFPs) are indispensable tools for deep-tissue imaging, fluorescence resonance energy transfer applications, and super-resolution microscopy. Using time-resolved optical spectroscopy this study investigated photoinduced dynamics of three RFPs, KillerRed, mRFP, and DsRed. In all three RFPs, a new transient absorption intermediate was observed, which decays on a microsecond-millisecond time scale. This intermediate is characterized by red-shifted absorption at 1.68-1.72 eV (λmax = 720-740 nm). On the basis of electronic structure calculations, experimental evidence, and published literature, the chemical nature of the intermediate is assigned to an unusual open-shell dianionic chromophore (dianion-radical) formed via photoreduction. A doubly charged state that is not stable in the isolated (gas phase) chromophore is stabilized by the electrostatic field of the protein. Mechanistic implications for photobleaching, blinking, and phototoxicity are discussed.

Obelia longissima, a tiny hydrozoan living in temperate and cold seas, features the Obelin photoprotein, which emits blue light. The Obelin bioluminescence and the Ca(2+)-discharged Obelin fluorescence spectra show multimodal characteristics that are currently interpreted by the concomitant participation of several light emitters. Up to now, the coelenteramide luminophore is thought to exist in different protonation states, one of them engaged in an ion-pair with the nearby residue, His22. Using hybrid quantum mechanics/molecular mechanics (QM/MM) calculations, we demonstrate that such an ion-pair cannot exist as a stable light emitter. However, when His22 electric neutrality is maintained by means of another proton transfer, the phenolate state of coelenteramide exhibits emission properties in agreement with experiment. Finally, an alternative nonradiative decay pathway, involving the formation of a diradical excited state, is postulated for the first time.

Fluorescent proteins have revolutionized molecular biology research and provide a means of tracking subcellular processes with extraordinary spatial and temporal precision. Species with emission beyond 650 nm offer the potential for deeper tissue penetration and lengthened imaging times; however, the origin of their extended Stokes shift is not fully understood. We employed spectrally resolved transient grating spectroscopy and molecular dynamics simulations to investigate the relationship between the flexibility of the chromophore environment and Stokes shift in mPlum. We examined excited state solvation dynamics in a panel of strategic point mutants of residues E16 and I65 proposed to participate in a hydrogen-bonding interaction thought responsible for its red-shifted emission. We observed two characteristic relaxation constants of a few picoseconds and tens of picoseconds that were assigned to survival times of direct and water-mediated hydrogen bonds at the 16-65 position. Moreover, variants of the largest Stokes shift (mPlum, I65V) exhibited significant decay on both time scales, indicating the bathochromic shift correlates with a facile switching between a direct and water-mediated hydrogen bond. This dynamic model underscores the role of environmental flexibility in the mechanism of excited state solvation and provides a template for engineering next-generation red fluorescent proteins.

The key events in the light-induced switching mechanism of the photochromic green fluorescent protein Padron have been investigated by employing femtosecond fluorescence up-conversion, femtosecond transient absorption, and time-correlated single photon counting techniques. In contrast to Dronpa, excitation of protein's neutral state at 395 nm triggers an efficient and complex photoswitching to a dark state whereas irradiation with 495 nm light reverses the protein to its initial state restoring the bright fluorescence. On the basis of the kinetics observed upon irradiation of the chromophore in the protonated state, we suggest that the switching mechanism consists of a light-initiated excited state process (presumably ESPT) with a time constant of 1 ps producing an unstable intermediate state, tentatively assigned to the excited state of the cis-anionic form, that is followed by a cis- to trans- isomerization (14.5 ps) forming the trans-anionic state in which the dark chromophore resides. In the trans-state, the protonation equilibrium strongly favors the anionic form. Consequently, upon excitation of the formed anionic species a trans-cis isomerization of the chromophore was found to occur with a time constant as fast as 5.2 ps switching the chromophore quantitatively to the bright (anionic) state.

Chromoprotein asFP595 and its A143G variant called kindling fluorescent protein (KFP) are among the chronologically first species for which trans-cis chromophore isomerization has been proposed as a driving force of photoswitching. In spite of long-lasting efforts to characterize the route between protein conformations referring to the trans and cis forms of the chromophore, the molecular mechanism of this transformation is still under debate. We report the results of computational studies of the trans-cis isomerization of the anionic and neutral chromophore inside the protein matrices in the ground electronic state for both variants, asFP595 and KFP. Corresponding free energy profiles (potentials of mean force) were evaluated by using molecular dynamics simulations with the quantum mechanical-molecular mechanical (QM/MM) forces. The computed free energy barrier for the cis-trans ground state (thermal) isomerization reaction is about 2 kcal/mol higher in KFP than that in asFP595. These results provide interpretation of experimental studies on thermal relaxation from the light-induced activation of fluorescence of these proteins and correctly show that the A143G mutation in asFP595 noticeably increases the lifetime of the fluorescence species.

Photochromic proteins, such as Dronpa, are of particular importance in bioimaging and form the basis of ultraresolution fluorescence microscopy. The photochromic reaction involves switching between a weakly emissive neutral trans form of the chromophore (A) and its emissive cis anion (B). Controlling the rates of switching has the potential to significantly enhance the spatial and temporal resolution in microscopy. However, the mechanism of the switching reaction has yet to be established. Here we report a high signal-to-noise ultrafast transient infrared investigation of the photochromic reaction in the mutant Dronpa2, which exhibits facile switching behavior. In these measurements we excite both the A and B forms and observe the evolution in the IR difference spectra over hundreds of picoseconds. Electronic excitation leads to bleaching of the ground electronic state and instantaneous (subpicosecond) changes in the vibrational spectrum of the protein. The chromophore and protein modes evolve with different kinetics. The chromophore ground state recovers in a fast nonsingle-exponential relaxation, while in a competing reaction the protein undergoes a structural change. This results in formation of a metastable form of the protein in its ground electronic state (A'), which subsequently evolves on the time scale of hundreds of picoseconds. The changes in the vibrational spectrum that occur on the subnanosecond time scale do not show unambiguous evidence for either proton transfer or isomerization, suggesting that these low-yield processes occur from the metastable state on a longer time scale and are thus not the primary photoreaction. Formation of A', and further relaxation of this state to the cis anion B, are relatively rare events, thus accounting for the overall low yield of the photochemical reaction.

Understanding bioluminescence presents fascinating challenges for fundamental sciences and numerous opportunities for practical applications. As a representative example, the firefly bioluminescent system has been intensively studied in both experimental and computational areas. However, there are still remaining questions regarding especially the detailed protein dynamics and the mechanisms of its color modulation. Here, we report on the pH dependent behavior of the firefly bioluminescence primarily based on molecular dynamics simulations. We find that the overall protein structure is generally resilient to pH variations. As the protein does not exhibit any structural distortions that can affect the emission property, we next focus on the dynamics in the active pocket and its effect on color modulation by adopting different protonation states in the pocket. With this, we observe red-shifted emissions at acidic conditions as consistent with previous studies. Most importantly, we find that a water molecule in the active pocket can mediate flexible motions of neighboring groups, which can subsequently modify the emission properties to a substantial degree. Based on the observations, we propose that the active pocket is in a dry condition during the luminescence process. Our results highlight the importance of understanding the role of the dynamics near the active pocket in modulating bioluminescence.

The kindling fluorescent protein (KFP), the Ala143Gly variant of the natural chromoprotein asFP595, is a prospective biomarker in live cells. Following the results of QM/MM calculations, we predict that excitation of the protein under certain conditions, favoring formation of KFP fractions with the neutral chromophore, should result in fluorescence from the cationic form of the chromophore which is unusual for the members of the green fluorescent protein family. Occurrence of the neutral form is due to a water wire connecting the chromophore with the exterior of the protein. Occurrence of the cationic form is due to the excited-state proton transfer from the conserved Glu215 to the imidazolinone ring nitrogen of the chromophore. The emission band from conformations with the trans cationic chromophore should be noticeably shifted to the blue side around 520 nm compared to the well-known red fluorescence around 600 nm arising from the cis anionic species.

The structural and functional plasticity of Aplysia mechanosensory presynaptic neurons has been studied in relation with the mechanism underlying learning and memory. Long-term facilitation (LTF), which is a well-known cellular model for long-term memory in Aplysia, is accompanied by new synaptic structural growth or change. We developed a combined atomic force microscope and confocal laser scanning microscope (AFM-CLSM) system integrated with a MATLAB routine for image processing to concurrently obtain high-resolution 3-dimensional (3D) outer-surface morphological images and 3D interior fluorescence images. With our combined AFM-CLSM system, volumetric changes in the presynaptic structures (varicosities) of Aplysia live sensory-motor neuron cocultures were observed. The spatial distribution of synaptic vesicle molecules in the preexisting varicosities was monitored together with a volumetric change in the varicosities. Our combined AFM-CLSM system is successfully adapted for measuring learning-related structural changes and the movement of synaptic molecules in the single live neuron through interaction force and fluorescence imaging.

Green-to-red photoconversion is a reaction that occurs in a limited number of fluorescent proteins and that is currently mechanistically debated. In this contribution, we report on our investigation of the photoconvertible fluorescent protein Dendra2 by employing a combination of pump-probe, up-conversion and single photon timing spectroscopic techniques. Our findings indicate that upon excitation of the neutral green state an excited state proton transfer proceeds with a time constant of 3.4 ps between the neutral green and the anionic green states. In concentrated solution we detected resonance energy transfer (25 ps time constant) between green and red monomers. The time-resolved emission spectra suggest also the formation of a super-red species, first observed for DsRed (a red fluorescent protein from the corallimorph species Discosoma) and consistent with peculiar structural details present in both proteins.

The development of fluorescent proteins (FPs) has revolutionized cell biology research. The monomeric variants of red fluorescent proteins (RFPs), known as mFruits, have been especially valuable for tagging and tracking cellular processes in vivo. Determining oxygen diffusion pathways in FPs can be important for improving photostability and for understanding maturation of the chromophore. We use molecular dynamics (MD) calculations to investigate the diffusion of molecular oxygen in one of the most useful monomeric RFPs, mCherry. We describe a pathway that allows oxygen molecules to enter from the solvent and travel through the protein barrel to the chromophore. We calculate the free-energy of an oxygen molecule at points along the path. The pathway contains several oxygen hosting pockets, which are identified by the amino acid residues that form the pocket. We also investigate an RFP variant known to be significantly less photostable than mCherry and find much easier oxygen access in this variant. The results provide a better understanding of the mechanism of molecular oxygen access into the fully folded mCherry protein barrel and provide insight into the photobleaching process in these proteins.

To determine the energetic feasibility of the mechanisms involved in the generation of the fluorescent species in red fluorescent proteins LSSmKate1 and LSSmKate2 developed by Piatkevich et al. (Proc. Natl. Acad. Sci. U.S.A. 2010, 107, 5369-5374 and J. Am. Chem. Soc. 2010, 132, 10762-10770), a potential energy scan for the respective reaction coordinates was performed in large cluster models including the surroundings of the chromophores, based on the respective crystallographic structures, using DFT and TDDFT. The predicted absorption wavelengths agree to within 5 nm with experiment, thus confirming the accuracy of the calculational level and modeling done. In both proteins, it was found that the adiabatic electronic state with the largest oscillator strength at the Franck-Condon region was not the one from which fluorescence could occur in the products. A diabatization procedure was used to determine an approximate photoactive state, based on selecting the state with the largest oscillator strength throughout. For LSSmKate1, this led to a rather flat potential energy profile but still did not predict a minimum in the product side. It is suggested that relaxation processes, absent from the model, could bring about such a minimum. LSSmKate2, on the other hand, clearly displays a favorable exoergic process in the photoactive state, and its double-proton transfer can be described as concerted but highly asynchronous, involving a barrier in the transfer of the first proton. In this way, the model provides strong support for the mechanism proposed for LSSmKate2.

Molecular dynamics calculations of pressure effects on mStrawberry and mCherry fluorescent proteins are reported. The simulations reveal that mStrawberry has much floppier structure at atmospheric pressure, as evidenced by larger backbone fluctuations and the coexistence of two conformers that differ by Ser146 orientation. Consequently, pressure increase has a larger effect on mStrawberry, making its structure more rigid and reducing the population of one of the conformers. The most significant effect of pressure increase is in the hydrogen-bonding network between the chromophore and the nearby residues. The quantum-mechanics/molecular mechanics calculations of excitation energies in mStrawberry explain the observed blue shift and identify Lys70 as the residue that has the most pronounced effect on the spectra. The results suggest that pressure increase causes an initial increase of fluorescence yield only for relatively floppy fluorescent proteins, whereas the fluorescent proteins that have more rigid structures have quantum yields close to their maximum. The results suggest that a low quantum yield in fluorescent proteins is dynamic in nature and depends on the range of thermal motions of the chromophore and fluctuations in the H-bonding network rather than on their average structure.

The excited state dynamics of the blue fluorescent protein (BFP) and its variants, azurite, EBFP1.2, and EBFP2.0, are studied using molecular dynamics (MD) simulations on potential energy surfaces (PESs) generated with the interpolated mechanics-molecular mechanics (IM/MM) scheme. This IM/MM strategy adopts the interpolated PES for an important area of the complex and the conventional force field for the remaining part. We focus on the internal rotation dynamics of the chromophore unit, which is directly related to its fluorescence property, and analyze the time evolutions of the nonrotated chromophore fractions based on trajectories over 10 μs of aggregate simulation time. The characteristics obtained from the calculated time progresses of the nonrotated chromophore fractions in BFP and other variants agree well with experimentally observed properties. The results show that the MD simulation with an IM/MM potential is an attractive approach for studying excited state dynamics of fluorescent proteins in consideration of its efficiency and reliability. We also attempt to investigate the detailed roles that the mutated residues play in delaying the excited state chromophore twisting and thus improving the fluorescence property, and discuss the contributions by the Coulombic and the steric interactions between the chromophore and the mutated residues.

We present an experimental study on the fluorescence behavior of the red fluorescent proteins TagRFP-S, TagRFP-T, mCherry, mOrange2, mStrawberry, and mKO as a function of pressure up to several GPa. TagRFP-S, TagRFP-T, mOrange2, and mStrawberry show an initial increase in fluorescence intensity upon application of pressure above ambient conditions. At higher pressures, the fluorescence intensity decreases dramatically for all proteins under study, probably due to denaturing of the proteins. Small blue shifts in the fluorescence spectra with increasing pressure were seen in all proteins under study, hinting at increased rigidity of the chromophore environment. In addition, mOrange2 and mStrawberry exhibit strong and abrupt changes in their fluorescence spectra at certain pressures. These changes are likely due to structural modifications of the hydrogen bonding environment of the chromophore. The strong differences in behavior between proteins with identical or very similar chromophores highlight how the chromophore environment contributes to pressure-induced behavior of the fluorescence performance.