Charge transfer in green fluorescent protein.

Charge transfer reactions that contribute to the photoreactions of the wild type green fluorescent protein (GFP) do not occur in the isolated p-hydroxybenzylidene-imidazolidinone chromophore, demonstrating the role of the protein environment. The high quantum efficiency of the fluorescence photocycle that includes excited state proton transfer and the suppression of non-radiative pathways by the protein environment have been correlated with structural dynamics in the chromophore environment. A low quantum efficiency competing phototransformation reaction of GFP is accompanied by both proton and electron transfer, and closely mimics the charge redistribution that is occurring in the fluorescence photocycle. The protein response to this destabilising event has been demonstrated by cryo-trapping of early products in the reaction pathway and is found to be strong even at 100 K, including displacements of chromophore, protein, solvent and a photogenerated CO2 molecule derived from the decarboxylated Glu 222 side chain. We discuss the ramifications of the observation of strong conformational perturbations below the protein dynamical transition at approximately 200 K, in view of low temperature work on other light sensitive proteins such as myoglobin and bacteriorhodopsin. The proton and electron transfer in the phototransformation pathway mimics the proton and charge transfer which occurs during the fluorescence cycle, which leads to common structural responses in both photoreactions as shown by ultrafast spectroscopy. We review and discuss literature on light-induced and thermal charge transfer events, focusing on recent findings addressing conformational dynamics and implications for thermodynamic properties.     

Structure, function, and wavelength selection in blue-absorbing proteorhodopsin

The absorption maximum of blue proteorhodopsin (BPR) is the most blue-shifted of all retinal proteins found in archaea or bacteria, with the exception of sensory rhodopsin II (SRII). The absorption spectrum also exhibits a pH dependence larger than any other retinal protein. We examine the structural origins of these two properties of BPR by using optical spectroscopy, homology modeling, and molecular orbital theory. Bacteriorhodopsin (BR) and SRII are used as homology parents for comparative purposes. We find that the tertiary structure of BPR based on SRII is more realistic with respect to free energy, dynamic stability, and spectroscopic properties. Molecular orbital calculations including full single- and double-configuration interaction within the chromophore pi-electron system provide perspectives on the wavelength regulation in this protein and indicate that Arg-95, Gln-106, Glu-143, and Asp-229 play important, and in some cases pH-dependent roles. A possible model for the 0.22 eV red shift of BPR at low pH is examined, in which Glu-143 becomes protonated and releases Arg-95 to rotate up into the binding site, altering the electrostatic environment of the chromophore. At high pH, BPR has spectroscopic properties similar to SRII, but at low pH, BPR has spectroscopic properties more similar to BR. Nevertheless, SRII is a significantly better homology model for BPR and opens up the question of whether this protein serves as a proton pump, as commonly believed, or is a light sensor with structure-function properties more comparable to those of SRII. The function of BPR in the native organism is discussed with reference to the results of the homology model.     

Molecular dynamics studies on mutants of Cu,Zn superoxide dismutase: The functional role of charged residues in the electrostatic loop VII

Molecular dynamics (MD) calculations have been performed on mutants of superoxide dismutase (SOD) on some residues present in the electrostatic loop. These calculations have provided the solution structures for the mutants Thr-137 → IIe and Arg; Lys-136 → Ala; Glu-132 → Gln; Glu-133 → Gln; Glu-132, Glu-133 → Gln-132, Gln-133 and → Gln-132, Lys-133. The structural and dynamic properties of these mutants have been correlated with the catalytic properties and available spectroscopic data. The water molecule present in the active site close to the copper ion in wild type (WT) SOD is missing in the MD average structure of the Thr-137 → IIe mutant, while this molecule is present in the MD average structures of all the other mutants and of WT SOD. This agrees with the experimental data. This is an important result that shows the validity of our calculations and their ability to reproduce even subtle structural features. Addition of one or more positive charges on the 132 and/or 133 positions does not sizably perturb the structure of the active site channel, while the introduction of a positively charged residue (Arg) on position 137 has a large effect on the structure of the electrostatic loop. Analysis of the MD average structures of these mutants has pointed out that the simple electrostatic effects of charged residues in the channel are not the only factor relevant for enzymatic behavior but that the structure of the electrostatic loop and the location of the charged residues also contribute to the catalytic properties of SOD. © 1994 John Wiley & Sons, Inc.     

An alternative excited-state proton transfer pathway in green fluorescent protein variant S205V

Wild-type green fluorescent protein (wt-GFP) has a prominent absorbance band centered at approximately 395 nm, attributed to the neutral chromophore form. The green emission arising upon excitation of this band results from excited-state proton transfer (ESPT) from the chromophore hydroxyl, through a hydrogen-bond network proposed to consist of a water molecule and Ser205, to Glu222. Although evidence for Glu222 as a terminal proton acceptor has already been obtained, no evidence for the participation of Ser205 in the proton transfer process exists. To examine the role of Ser205 in the proton transfer, we mutated Ser205 to valine. However, the derived GFP variant S205V, upon excitation at 400 nm, still produces green fluorescence. Time-resolved emission spectroscopy suggests that ESPT contributes to the green fluorescence, and that the proton transfer takes place approximately 30 times more slowly than in wt-GFP. The crystal structure of S205V reveals rearrangement of Glu222 and Thr203, forming a new hydrogen-bonding network. We propose this network to be an alternative ESPT pathway with distinctive features that explain the significantly slowed rate of proton transfer. In support of this proposal, the double mutant S205V/T203V is shown to be a novel blue fluorescent protein containing a tyrosine-based chromophore, yet is incapable of ESPT. The results have implications for the detailed mechanism of ESPT and the photocycle of wt-GFP, in particular for the structures of spectroscopically identified intermediates in the cycle.     

Diverse roles of glycine residues conserved in photoactive yellow proteins

The role of glycine residues was studied by alanine-scanning mutagenesis using photoactive yellow protein, a structural prototype of PER ARNT SIM domain proteins, as a template. Mutation of glycine located close to the end of beta-strands with dihedral angles disallowed for alanine (Gly-37, Gly-59, Gly-86, and Gly-115) induces destabilization of the protein structure. On the other hand, substitution for Gly-77 and Gly-82, incorporated into the fifth alpha-helix, slows the photocycle by 15-20 times, suggesting that these residues regulate the light-induced structural switch between dark-state structure and signaling-state structure. Most importantly, a significant amount of G29A is in the bleached state and showed a 1000-fold slower photocycle. As O(epsilon2) of the carboxylic acid of Glu-46 is close enough for contact with C(alpha) of Gly-29, alanine mutation perturbs this packing. Fourier transform infrared spectroscopy demonstrated that the C=O(epsilon2) stretching mode of Glu-46 is 6 cm(-1) upshifted in G29A, suggesting that C(alpha) of Gly-29 acts as a proton donor for the C(alpha)-H...O(epsilon2) hydrogen bond with Glu-46, which stabilizes the dark-state structure. During the photocycle, Glu-46 becomes negatively charged by donating a proton to the chromophore, resulting in breakage of this hydrophobic packing and consequent conformational change of the protein.     

Water structural changes involved in the activation process of photoactive yellow protein

Fourier transform infrared (FTIR) spectroscopy was applied to the blue-light photoreceptor photoactive yellow protein (PYP) to investigate water structural changes possibly involved in the photocycle of PYP. Photointermediates were stabilized at low temperature, and difference IR spectra were obtained between intermediate states and the original state of PYP (pG). Water structural changes were never observed in the >3570 cm(-)(1) region for the intermediates stabilized at 77-250 K, such as the red-shifted pR and blue-shifted pB intermediates. In contrast, a negative band was observed at 3658 cm(-)(1) in the pB minus pG spectrum at 295 K, which shifts to 3648 cm(-)(1) upon hydration with H(2)(18)O. The high frequency of the O-H stretch of water indicates that the water O-H group does not form hydrogen bonds in pG, and newly forms these upon pB formation at 295 K, but not at 250 K. Among 92 water molecules in the crystal structure of PYP, only 1 water molecule, water-200, is present in a hydrophobic core inside the protein. The amide N-H of Gly-7 and the imidazole nitrogen atom of His-108 are its possible hydrogen-bonding partners, indicating that one O-H group of water-200 is free to form an additional hydrogen bond. The water band at 3658 cm(-)(1) was indeed diminished in the H108F protein, which strongly suggests that the water band originates from water-200. Structural changes of amide bands in pB were much greater in the wild-type protein at 295 K than at 250 K or in the H108F protein at 295 K. The position of water-200 is >15 A remote from the chromophore. Virtually no structural changes were reported for regions larger than a few angstroms away from the chromophore, in the time-resolved X-ray crystallography experiments on pB. On the basis of the present results, as well as other spectroscopic observations, we conclude that water-200 (buried in a hydrophobic core in pG) is exposed to the aqueous phase upon formation of pB in solution. In neither crystalline PYP nor at low temperature is this structural transition observed, presumably because of the restrictions on global structural changes in the protein under these conditions.     

Balance between ultrafast parallel reactions in the green fluorescent protein has a structural origin

The fluorescence photocycle of the green fluorescent protein is functionally dependent on the specific structural protein environment. A direct relationship between equilibrium protein side-chain conformation of glutamate 222 and reactivity is established, particularly the rate of ultrafast proton transfer reactions in the fluorescence photocycle. We show that parallel transformations in the photocycle have a structural origin, and we report on the vibrational properties of responsive amino acids on an ultrafast timescale. Blue excitation of GFP drives two parallel, excited-state deuteron transfer reactions with 10 ps and 75 ps time constants to the buried carboxylic acid side chain of glutamate 222 via a hydrogen-bonding network. Assignment of 1456 cm⁻¹ and 1441 cm⁻¹ modes to ν_sym and assignment of 1564 cm⁻¹ and 1570 cm⁻¹ features to ν_asym of E222 in the 10 ps and 75 ps components, respectively, was possible from the analysis of the transient absorption data of an E222D mutant and was consistent with photoselection measurements. In contrast to the wild-type, measurements of E222D can be described with only one difference spectrum, with the ν_sym mode at 1435 cm⁻¹ and the ν_asym mode at 1567 cm⁻¹, also correlating a large Δν_asym-sym with slow excited-state proton transfer kinetics. Density Functional Theory calculations and published model compound and theoretical studies relate differences in Δν_asym-sym to the strength and number of hydrogen-bonding interactions that are detected via equilibrium geometry and COO⁻ stretching frequency differences of the carboxylate. The correlation of photocycle kinetics with side-chain conformation of the acceptor suggests that proton transfer from S205 to E222 controls the rate of the overall excited-state proton transfer process, which is consistent with recent theoretical predictions. Photoselection measurements show agreement for localized CO vibrations of chromophore, Q69, and E222 with Density Functional Theory and ab initio calculations placed in the x-ray geometry and provide their vibrational response in the intermediates in the photocycle.     

Electric-field dependent decays of two spectroscopically different M-states of photosensory rhodopsin II from Natronobacterium pharaonis

Sensory rhodopsin II (NpSRII) from Natronobacterium pharaonis was studied by resonance Raman (RR) spectroscopic techniques. Using gated 413-nm excitation, time-resolved RR measurements of the solubilized photoreceptor were carried out to probe the photocycle intermediates that are formed in the submillisecond time range. For the first time, two M-like intermediates were identified on the basis of their C=C stretching bands at 1568 and 1583 cm(-1), corresponding to the early M(L)(400) state with a lifetime of 30 micro s and the subsequent M(1)(400) state with a lifetime of 2 ms, respectively. The unusually high C=C stretching frequency of M(1)(400) has been attributed to an unprotonated retinal Schiff base in a largely hydrophobic environment, implying that the M(L)(400) --> M(1)(400) transition is associated with protein structural changes in the vicinity of the chromophore binding pocket. Time-resolved surface enhanced resonance Raman experiments of NpSRII electrostatically bound onto a rotating Ag electrode reveal that the photoreceptor runs through the photocycle also in the immobilized state. Surface enhanced resonance Raman spectra are very similar to the RR spectra of the solubilized protein, ruling out adsorption-induced structural changes in the retinal binding pocket. The photocycle kinetics, however, is sensitively affected by the electrode potential such that at 0.0 V (versus Ag/AgCl) the decay times of M(L)(400) and M(1)(400) are drastically slowed down. Upon decreasing the potential to -0.4 V, that corresponds to a decrease of the interfacial potential drop and thus of the electric field strength at the protein binding site, the photocycle kinetics becomes similar to that of NpSRII in solution. The electric-field dependence of the protein structural changes associated with the M-state transitions, which in the present spectroscopic work is revealed on a molecular level, appears to be related to the electric-field control of bacteriorhodopsin's photocycle, which has been shown to be of functional relevance.     

Transition in the temperature-dependence of GFP fluorescence: from proton wires to proton exit

In green fluorescent protein, photo-excitation leads to excited-state proton transfer from its chromophore, leaving behind a strongly fluorescing anion, while the proton is commonly thought to migrate internally to Glu-222. X-ray data show that the protein contains more extended hydrogen-bonded networks that can support proton migration (i.e., proton wires). Here we study the temperature-dependence of the transient fluorescence from both the acid and anionic forms up to 15 ns. At low temperatures, we find that the (lifetime-corrected) fluorescence of the acidic form decays asymptotically as t^−1/2, following quantitatively the solution of a one-dimensional diffusion equation for reversible geminate recombination with quenching. This indicates proton migration along the internal proton wires. A small degree of geminate proton quenching is attributed to the formation of the zwitterion by proton migration on a side-branch of the proton wire. Above 230 K, the fluorescence kinetics undergo a transition, exhibiting an asymptotic t^−3/2 decay, and the quenching effect disappears. We interpret these findings as evidence for a conformational change enabling the rotation of Thr-203, which eventually allows the proton to escape to the exterior solution.     

A molecular movie at 1.8 A resolution displays the photocycle of photoactive yellow protein, a eubacterial blue-light receptor, from nanoseconds to seconds.

The photocycle of the bacterial blue-light photoreceptor, photoactive yellow protein, was stimulated by illumination of single crystals by a 7 ns laser pulse. The molecular events were recorded at high resolution by time-resolved X-ray Laue diffraction as they evolved in real time, from 1 ns to seconds after the laser pulse. The complex structural changes during the photocycle at ambient temperature are displayed in a movie of difference electron density maps relative to the dark state. The step critical to entry into the photocycle is identified as flipping of the carbonyl group of the 4-hydroxycinnamic acid chromophore into an adjacent, hydrophobic environment rather than the concomitant isomerization about the double bond of the chromophore tail. The structural perturbation generated at the chromophore propagates throughout the entire protein as a light-induced "protein quake" with its "epicenter" at the carbonyl moiety of the chromophore.     

Fourier transform infrared study of the halorhodopsin chloride pump

Halorhodopsin (hR) is a light-driven chloride pump located in the cell membrane of Halobacterium halobium. Fourier transform infrared difference spectroscopy has been used to study structural alterations occurring during the hR photocycle. The frequencies of peaks attributed to the retinylidene chromophore are similar to those observed in the spectra of the related protein bacteriorhodopsin (bR), indicating that in hR as in bR an all-trans----13-cis isomerization occurs during formation of the early bathoproduct. Spectral features due to protein structural alterations are also similar for the bR and hR photocycles. For example, formation of the red-shifted primary photoproducts of both hR and bR results in similar carboxyl peaks in the 1730-1745-cm-1 region. However, in contrast to bR, no further changes are observed in the carboxyl region during subsequent steps in the hR photocycle, indicating that additional carboxyl groups are not directly involved in chloride translocation. Overall, the close similarity of vibrations in hR and bR photoproduct difference spectra supports the existence of some common elements in the molecular mechanisms of energy transduction and active transport by these two proteins.     

Photochemical reaction cycle and proton transfers in Neurospora rhodopsin.

It was recently found that NOP-1, a membrane protein of Neurospora crassa, shows homology to haloarchaeal rhodopsins and binds retinal after heterologous expression in Pichia pastoris. We report on spectroscopic properties of the Neurospora rhodopsin (NR). The photocycle was studied with flash photolysis and time-resolved Fourier-transform infrared spectroscopy in the pH range 5-8. Proton release and uptake during the photocycle were monitored with the pH-sensitive dye, pyranine. Kinetic and spectral analysis revealed six distinct states in the NR photocycle, and we describe their spectral properties and pH-dependent kinetics in the visible and infrared ranges. The phenotypes of the mutant NR proteins, D131E and E142Q, in which the homologues of the key carboxylic acids of the light-driven proton pump bacteriorhodopsin, Asp-85 and Asp-96, were replaced, show that Glu-142 is not involved in reprotonation of the Schiff base but Asp-131 may be. This implies that, if the NR photocycle is associated with proton transport, it has a low efficiency, similar to that of haloarchaeal sensory rhodopsin II. Fourier-transform Raman spectroscopy revealed unexpected differences between NR and bacteriorhodopsin in the configuration of the retinal chromophore, which may contribute to the less effective reprotonation switch of NR.     

Aspartate 75 mutation in sensory rhodopsin II from Natronobacterium pharaonis does not influence the production of the K-like intermediate, but strongly affects its relaxation pathway

The early steps in the photocycle of the aspartate 75-mutated sensory rhodopsin II from Natrobacterium pharaonis (pSRII-D75N) were studied by time-resolved laser-induced optoacoustic spectroscopy combined with quantum yield determinations by flash photolysis with optical detection. Similar to the case of pSRII-WT, excitation of pSRII-D75N produces in subnanosecond time a K-like intermediate. Different to the case of K in pSRII-WT, in pSRII-D75N there are two K states. K(E) decays into K(L) with a lifetime of 400 ns (independent of temperature in the range 6.5-52 degrees C) which is optically silent under the experimental conditions of our transient absorption experiments. This decay is concomitant with an expansion of 6.5 ml/mol of produced intermediate. This indicates a protein relaxation not affecting the chromophore absorption. For pSRII-D75N reconstituted into polar lipids from purple membrane, the mutation of Asp-75 by the neutral residue Asn affects neither the K(E) production yield (PhiK(e) 0.51 +/- 0.05) nor the energy stored by this intermediate (E(E)K(E) = 91 +/- 11 kJ/mol), nor the expansion upon its production (DeltaV(R,1) = 10 +/- 0.3 ml/mol). All these values are very similar to those previously determined for K with pSRII-WT in the same medium. The millisecond transient species is attributed to K(L) with a lifetime corresponding to that determined by electronic absorption spectroscopy for K(565). The determined energy content of the intermediates as well as the structural volume changes for the various steps afford the calculation of the free energy profile of the phototransformation during the pSRII-D75N photocycle. These data offer insights regarding the photocycle in pSRII-WT. Detergent solubilization of pSRII-D75N affects the sample properties to a larger extent than in the case of pSRII-WT.     

Conformational changes in the photocycle of Anabaena sensory rhodopsin: absence of the Schiff base counterion protonation signal

Anabaena sensory rhodopsin (ASR) is a novel microbial rhodopsin recently discovered in the freshwater cyanobacterium Anabaena sp. PCC7120. This protein most likely functions as a photosensory receptor as do the related haloarchaeal sensory rhodopsins. However, unlike the archaeal pigments, which are tightly bound to their cognate membrane-embedded transducers, ASR interacts with a soluble cytoplasmic protein analogous to transducers of animal vertebrate rhodopsins. In this study, infrared spectroscopy was used to examine the molecular mechanism of photoactivation in ASR. Light adaptation of the pigment leads to a phototransformation of an all-trans/15-anti to 13-cis/15-syn retinylidene-containing species very similar in chromophore structural changes to those caused by dark adaptation in bacteriorhodopsin. Following 532 nm laser-pulsed excitation, the protein exhibits predominantly an all-trans retinylidene photocycle containing a deprotonated Schiff base species similar to those of other microbial rhodopsins such as bacteriorhodopsin, sensory rhodopsin II, and Neurospora rhodopsin. However, no changes are observed in the Schiff base counterion Asp-75, which remains unprotonated throughout the photocycle. This result along with other evidence indicates that the Schiff base proton release mechanism differs significantly from that of other known microbial rhodopsins, possibly because of the absence of a second carboxylate group at the ASR photoactive site. Several conformational changes are detected during the ASR photocycle including in the transmembrane helices E and G as indicated by hydrogen-bonding alterations of their native cysteine residues. In addition, similarly to animal vertebrate rhodopsin, perturbations of the polar head groups of lipid molecules are detected.     

Spectroscopic properties and chromophore conformations of the photomorphogenic receptor: phytochrome.

Fluorescence lifetimes of 'large (mol. wt. 120,000) and 'small' (mol. wt. 60,000) phytochromes isolated from oat and rye seedlings grown in the dark have been measured at 199 K and 298 K. Phytochrome model compounds have also been studied by phase modulation fluorometrically at 77 K for comparison with lifetime data for phytochrome. It was found that the fluorescence lifetime of 'large' phytochrome was significantly shorter than that of 'small' phytochrome and its chromophore models. The phytochrome chromophore of Pr form has been analyzed by fluorescence polarization, CD, and molecular orbital methods. The fluorescence excitation polarization of 'small' phytochrome and the chromophore model in buffer/glycerol mixture (3 : 1, v/v) at 77 K is very hight (0.4) at the main absorption band and is negative (--0.1) and close to 0 in the near ultraviolet band, respectively. Analyses of the spectroscopic data suggest that the chromophore conformation of Pr and Pfr forms of phytochrome are essentially identical. The induced ellipticity of 'large' rye phytochrome in the blue and near ultraviolet regions was found to be significantly higher than that of 'small' phytochrome, indicating that the binding interaction between the phytochrome chromophore and apoprotein is much tighter in the former than in the latter. In addition, the excitation energy transfer does occur from Trp residue(s) to the chromophore in 'large' phytochrome but not in 'small' Pr. This illustrates one feature of the role played by the large molecular weight apoprotein in the binding site interactions and primary photoprocesses of Pr. Finally, a plausible model for the primary photoprocesses and the mechanism of phytochrome interactions triggered by the Pr leads to Pfr phototransformation have been proposed on the basis of the above results.     

A structural pathway for signaling in the E46Q mutant of photoactive yellow protein

In the bacterial photoreceptor photoactive yellow protein (PYP), absorption of blue light by its chromophore leads to a conformational change in the protein associated with differential signaling activity, as it executes a reversible photocycle. Time-resolved Laue crystallography allows structural snapshots (as short as 150 ps) of high crystallographic resolution (approximately 1.6 A) to be taken of a protein as it functions. Here, we analyze by singular value decomposition a comprehensive time-resolved crystallographic data set of the E46Q mutant of PYP throughout the photocycle spanning 10 ns-100 ms. We identify and refine the structures of five distinct intermediates and provide a plausible chemical kinetic mechanism for their inter conversion. A clear structural progression is visible in these intermediates, in which a signal generated at the chromophore propagates through a distinct structural pathway of conserved residues and results in structural changes near the N terminus, over 20 A distant from the chromophore.     

The nature of the primary photochemical events in rhodopsin and isorhodopsin.

The nature of the primary photochemical events in rhodopsin and isorhodopsin is studied by using low temperature actinometry, low temperature absorption spectroscopy, and intermediate neglect of differential overlap including partial single and double configuration interaction (INDO-PSDCI) molecular orbital theory. The principal goal is a better understanding of how the protein binding site influences the energetic, photochemical, and spectroscopic properties of the bound chromophore. Absolute quantum yields for the isorhodopsin (I) to bathorhodopsin (B) phototransformation are assigned at 77 K by using the rhodopsin (R) to bathorhodopsin phototransformation as an internal standard (phi R----B = 0.67). In contrast to rhodopsin photochemistry, isorhodopsin displays a wavelength dependent quantum yield for photochemical generation of bathorhodopsin at 77 K. Measurements at seven wavelengths yielded values ranging from a low of 0.089 +/- 0.021 at 565 nm to a high of 0.168 +/- 0.012 at 440 nm. An analysis of these data based on a variety of kinetic models suggests that the I----B phototransformation encounters a small activation barrier (approximately 0.2 kcal mol-1) associated with the 9-cis----9-trans excited-state torsional-potential surface. The 9-cis retinal chromophore in solution (EPA, 77 K) has the smallest oscillator strength relative to the other isomers: 1.17 (all-trans), 0.98 (9-cis), 1.04 (11-cis), and 1.06 (13-cis). The effect of conformation is quite different for the opsin-bound chromophores. The oscillator strength of the lambda max absorption band of I is observed to be anomalously large (1.11) relative to the lambda max absorption bands of R (0.98) and B (1.07). The wavelength-dependent photoisomerization quantum yields and the anomalous oscillator strength associated with isorhodopsin provide important information on the nature of the opsin binding site. Various models of the binding site were tested by using INDO-PSDCI molecular orbital theory to predict the oscillator strengths of R, B, and I and to calculate the barriers and energy storage associated with the photochemistry of R and I for each model. Our experimental and theoretical investigation leads to the following conclusions: (a) The counterion (abbreviated as CTN) is not intimately associated with the imine proton in R, B, or I. The counterion lies underneath the plane of the chromophore in R and I, and the primary chromophore-counterion electrostatic interactions involve C15-CTN and C13-CTN. These interactions are responsible for the anomalous oscillator strength of I relative to R and B.(ABSTRACT TRUNCATED AT 400 WORDS)     

Protonation/deprotonation reactions triggered by photoactivation of photoactive yellow protein from Ectothiorhodospira halophila.

Light-dependent pH changes were measured in unbuffered solutions of wild type photoactive yellow protein (PYP) and its H108F and E46Q variants, using two independent techniques: transient absorption changes of added pH indicator dyes and direct readings with a combination pH electrode. Depending on the absolute pH of the sample, a reversible protonation as well as a deprotonation can be observed upon formation of the transient, blue-shifted photocycle intermediate (pB) of this photoreceptor protein. The latter is observed at very alkaline pH, the former at acidic pH values. At neutral pH, however, the formation of the pB state is not paralleled by significant protonation/deprotonation of PYP, as expected for concomitant protonation of the chromophore and deprotonation of Glu-46 during pB formation. We interpret these results as further evidence that a proton is transferred from Glu-46 to the coumaric acid chromophore of PYP, during pB formation. One cannot exclude the possibility, however, that this transfer proceeds through the bulk aqueous phase. Simultaneously, an amino acid side chain(s) (e.g. His-108) changes from a buried to an exposed position. These results, therefore, further support the idea that PYP significantly unfolds in the pB state and resolve the controversy regarding proton transfer during the PYP photocycle.     

Structural and spectral response of green fluorescent protein variants to changes in pH

The green fluorescent protein (GFP) from the jellyfish Aequorea victoria has become a useful tool in molecular and cell biology. Recently, it has been found that the fluorescence spectra of most mutants of GFP respond rapidly and reversibly to pH variations, making them useful as probes of intracellular pH. To explore the structural basis for the titration behavior of the popular GFP S65T variant, we determined high-resolution crystal structures at pH 8.0 and 4.6. The structures revealed changes in the hydrogen bond pattern with the chromophore, suggesting that the pH sensitivity derives from protonation of the chromophore phenolate. Mutations were designed in yellow fluorescent protein (S65G/V68L/S72A/T203Y) to change the solvent accessibility (H148G) and to modify polar groups (H148Q, E222Q) near the chromophore. pH titrations of these variants indicate that the chromophore pKa can be modulated over a broad range from 6 to 8, allowing for pH determination from pH 5 to pH 9. Finally, mutagenesis was used to raise the pKa from 6.0 (S65T) to 7.8 (S65T/H148D). Unlike other variants, S65T/H148D exhibits two pH-dependent excitation peaks for green fluorescence with a clean isosbestic point. This raises the interesting possibility of using fluorescence at this isosbestic point as an internal reference. Practical real time in vivo applications in cell and developmental biology are proposed.     

Conservative mutations of glutamine-125 in herpes simplex virus type 1 thymidine kinase result in a ganciclovir kinase with minimal deoxypyrimidine kinase activities

The herpes simplex virus type 1 thymidine kinase (HSV-1 TK) is the major anti-herpes virus pharmacological target, and it is being utilized in combination with the prodrug ganciclovir as a toxin gene therapeutic for cancer. One active-site amino acid, glutamine-125 (Gln-125), has been shown to form hydrogen bonds with bound thymidine, thymidylate, and ganciclovir in multiple X-ray crystal structures. To examine the role of Gln-125 in HSV-1 TK activity, three site-specific mutations of this residue to an aspartic acid, an asparagine, or a glutamic acid were introduced. These three mutants and wild-type HSV-1 TK were expressed in E. coli and partially purified and their enzymatic properties compared. In comparison to the Gln-125 HSV-1 TK, thymidylate kinase activity of all three mutants was decreased by over 90%. For thymidine kinase activity relative to Gln-125 enzyme, the K(m) of thymidine increased from 0.9 microM for the parent Gln-125 enzyme to 3 microM for the Glu-125 mutant, to 6000 microM for the Asp-125 mutant, and to 20 microM for the Asn-125 mutant. In contrast, the K(m) of ganciclovir decreased from 69 microM for the parent Gln-125 enzyme to 50 microM for the Asn-125 mutant and increased to 473 microM for the Glu-125 mutant. The Asp-125 enzyme was able to poorly phosphorylate ganciclovir, but with nonlinear kinetics. Molecular simulations of the wild-type and mutant HSV-1 TK active sites predict that the observed activities are due to loss of hydrogen bonding between thymidine and the mutant amino acids, while the potential for hydrogen bonding remains intact for ganciclovir binding. When expressed in two mammalian cell lines, the Glu-125 mutant led to GCV-mediated killing of one cell line, while the Asn-125 mutant was equally as effective as wild-type HSV-1 TK in metabolizing GCV and causing cell death in both cell lines.