Photokinetic, biochemical and structural features of chimeric photoactive yellow protein constructs.

Of the 10 photoactive yellow protein (PYPs) that have been characterized, the two from Rhodobacter species are the only ones that have an additional intermediate spectral form in the resting state (λmax  = 375 nm), compared to the prototypical Halorhodospira halophila PYP. We have constructed three chimeric PYP proteins by replacing the first 21 residues from the N-terminus (Hyb1PYP), 10 from the ß4-ß5 loop (Hyb2PYP) and both (Hyb3PYP) in Hhal PYP with those from Rb. capsulatus PYP. The N-terminal chimera behaves both spectrally and kinetically like Hhal PYP, indicating that the Rcaps N-terminus folds against the core of Hhal PYP. A small fraction shows dimerization and slower recovery, possibly due to interaction at the N-termini. The loop chimera has a small amount of the intermediate spectral form and a photocycle that is 20 000 times slower than Hhal PYP. The third chimera, with both regions exchanged, resembles Rcaps PYP with a significant amount of intermediate spectral form (λmax  = 380 nm), but has even slower kinetics. The effects are not strictly additive in the double chimera, suggesting that what perturbs one site, affects the other as well. These chimeras suggest that the intermediate spectral form has its origins in overall protein stability and solvent exposure.

Tyrosine triad at the interface between the Rieske iron-sulfur protein, cytochrome c1 and cytochrome c2 in the bc1 complex of Rhodobacter capsulatus.

A triad of tyrosine residues (Y152-154) in the cytochrome c(1) subunit (C1) of the Rhodobacter capsulatus cytochrome bc(1) complex (BC1) is ideally positioned to interact with cytochrome c(2) (C2). Mutational analysis of these three tyrosines showed that, of the three, Y154 is the most important, since its mutation to alanine resulted in significantly reduced levels, destabilization, and inactivation of BC1. A second-site revertant of this mutant that regained photosynthetic capacity was found to have acquired two further mutations-A181T and A200V. The Y152Q mutation did not change the spectral or electrochemical properties of C1, and showed wild-type enzymatic C2 reduction rates, indicating that this mutation did not introduce major structural changes in C1 nor affect overall activity. Mutations Y153Q and Y153A, on the other hand, clearly affect the redox properties of C1 (e.g. by lowering the midpoint potential as much as 117 mV in Y153Q) and the activity by 90% and 50%, respectively. A more conservative Y153F mutant on the other hand, behaves similarly to wild-type. This underscores the importance of an aromatic residue at position Y153, presumably to maintain close packing with P184, which modeling indicates is likely to stabilize the sixth heme ligand conformation.

Occurrence and sequence of Sphaeroides Heme Protein and diheme cytochrome C in purple photosynthetic bacteria in the family Rhodobacteraceae.

BACKGROUND: Sphaeroides Heme Protein (SHP) was discovered in the purple photosynthetic bacterium, Rhodobacter sphaeroides, and is the only known c-type heme protein that binds oxygen. Although initially not believed to be widespread among the photosynthetic bacteria, the gene has now been found in more than 40 species of proteobacteria and generally appears to be regulated. Rb. sphaeroides is exceptional in not having regulatory genes associated with the operon. We have thus analyzed additional purple bacteria for the SHP gene and examined the genetic context to obtain new insights into the operon, its distribution, and possible function. RESULTS: We found SHP in 9 out of 10 strains of Rb. sphaeroides and in 5 out of 10 purple photosynthetic bacterial species in the family Rhodobacteraceae. We found a remarkable similarity within the family including the lack of regulatory genes. Within the proteobacteria as a whole, SHP is part of a 3-6 gene operon that includes a membrane-spanning diheme cytochrome b and one or two diheme cytochromes c. Other genes in the operon include one of three distinct sensor kinase - response regulators, depending on species, that are likely to regulate SHP. CONCLUSIONS: SHP is not as rare as generally believed and has a role to play in the photosynthetic bacteria. Furthermore, the two companion cytochromes along with SHP are likely to function as an electron transfer pathway that results in the reduction of SHP by quinol and formation of the oxygen complex, which may function as an oxygenase. The three distinct sensors suggest at least as many separate functional roles for SHP. Two of the sensors are not well characterized, but the third is homologous to the QseC quorum sensor, which is present in a number of pathogens and typically appears to regulate genes involved in virulence.

Regulation of the Ppr histidine kinase by light-induced interactions between its photoactive yellow protein and bacteriophytochrome domains.

Ppr is a unique bacteriophytochrome that bleaches rather than forming a far-red-shifted Pfr state upon red light activation. Ppr is also unusual in that it has a blue light photoreceptor domain, PYP, which is N-terminally fused to the bacteriophytochrome domain (Bph). When both photoreceptors are activated by light, the fast phase of Bph recovery (1 min lifetime) corresponds to the formation of an intramolecular long-lived complex between the activated PYP domain and the Bph domain (lifetime of 2-3 days). Since this state is unusually long-lived as compared to other intermediates in the photocycle of both PYP and Bph, we interpret this as formation of a metastable complex between activated PYP and Bph domains that takes days to relax. In the metastable complex, the PYP domain is locked in its activated UV absorbing state and the Bph domain is in a slightly red-shifted state (from 701 to 702 nm), which is photochemically inactive to red or white light. The amount of metastable complex formed increases with the degree of prior activation of PYP, reaching a maximum of 50% when PYP is fully activated compared to 0% when no PYP is activated. The saturation of complex formation at 50% is believed to be due to light-induced heterogeneity within the Ppr dimer. UV irradiation (365 nm) of the metastable complex state photoreverses the activated PYP and the red-shifted Bph to the initial dark state within seconds. We therefore postulate that Ppr functions as a UV-red light sensor and describe the different Ppr states that can be obtained depending on the light quality. Both red and white light upregulate the autokinase activity, while it is downregulated in the dark. The physiological state of Ppr is most likely a mixture of three different states, dark, metastable complex, and red light-activated, with fractional populations whose amounts depend on the light quality of the environment and that regulate the extent of phosphorylation by the kinase.

Strong hydrogen bond between glutamic acid 46 and chromophore leads to the intermediate spectral form and excited state proton transfer in the Y42F mutant of the photoreceptor photoactive yellow protein.

In the Y42F mutant of photoactive yellow protein (PYP) the photoreceptor is in an equilibrium between two dark states, the yellow and intermediate spectral forms, absorbing at 457 and 390 nm, respectively. The nature of this equilibrium and the light-induced protonation and structural changes in the two spectral forms were characterized by transient absorption, fluorescence, FTIR, and pH indicator dye experiments. In the yellow form, the oxygen of the deprotonated p-hydroxycinnamoyl chromophore is linked by a strong low-barrier hydrogen bond to the protonated carboxyl group of Glu46 and by a weaker one to Thr50. Using FTIR, we find that the band due to the carbonyl of the protonated side chain of Glu46 is shifted from 1736 cm(-1) in wild type to 1724 cm(-1) in the yellow form of Y42F, implying a stronger hydrogen bond with the deprotonated chromophore in Y42F. The FTIR data suggest moreover that in the intermediate spectral form the chromophore is protonated and Glu46 deprotonated. Flash spectroscopy (50 ns-10 s) shows that the photocycles of the two forms are essentially the same except for a transition around 5 mus that has opposite signs in the two forms and is due to the chemical relaxation between the two dark states. The two cycles are coupled, likely by excited state proton transfer. The Y42F cycle differs from wild type by the occurrence of a new intermediate with protonated chromophore between the usual I(1) and I(2) intermediates which we call I(1)H (370 nm). Transient fluorescence measurements indicate that in I(1)H the chromophore retains the orientation it had in I(1). Transient proton uptake occurs with a time constant of 230 mus and a stoichiometry of 1. No proton uptake was associated however with the formation of the I(1)H intermediate and the relaxation of the yellow/intermediate equilibrium. These protonation changes of the chromophore thus occur intramolecularly. The chromophore-Glu46 hydrogen bond in Y42F is shorter than in wild type, since the adjacent chromophore-Y42 hydrogen bond is replaced by a longer one with Thr50. This facilitates proton transfer from Glu46 to the chromophore in the dark by lowering the barrier, leading to the protonation equilibrium and causing the rapid light-induced proton transfer which couples the cycles.

Time-resolved spectroscopy of dye-labeled photoactive yellow protein suggests a pathway of light-induced structural changes in the N-terminal cap.

The photoreceptor PYP responds to light activation with global conformational changes. These changes are mainly located in the N-terminal cap of the protein, which is approximately 20 A away from the chromophore binding pocket and separated from it by the central beta-sheet. The question of the propagation of the structural change across the central beta-sheet is of general interest for the superfamily of PAS domain proteins, for which PYP is the structural prototype. Here we measured the kinetics of the structural changes in the N-terminal cap by transient absorption spectroscopy on the ns to second timescale. For this purpose the cysteine mutants A5C and N13C were prepared and labeled with thiol reactive 5-iodoacetamidofluorescein (IAF). A5 is located close to the N-terminus, while N13 is part of helix alpha1 near the functionally important salt bridge E12-K110 between the N-terminal cap and the central anti-parallel beta-sheet. The absorption spectrum of the dye is sensitive to its environment, and serves as a sensor for conformational changes near the labeling site. In both labeled mutants light activation results in a transient red-shift of the fluorescein absorption spectrum. To correlate the conformational changes with the photocycle intermediates of the protein, we compared the kinetics of the transient absorption signal of the dye with that of the p-hydroxycinnamoyl chromophore. While the structural change near A5 is synchronized with the rise of the I(2) intermediate, which is formed in approximately 200 mus, the change near N13 is delayed and rises with the next intermediate I(2)', which forms in approximately 2 ms. This indicates that different parts of the N-terminal cap respond to light activation with different kinetics. For the signaling pathway of photoactive yellow protein we propose a model in which the structural signal propagates from the chromophore binding pocket across the central beta-sheet via the N-terminal region to helix alpha1, resulting in a large change in the protein conformation.

Distinguishing chromophore structures of photocycle intermediates of the photoreceptor PYP by transient fluorescence and energy transfer.

The cinnamoyl chromophore is the light-activated switch of the photoreceptor photoactive yellow protein (PYP) and isomerizes during the functional cycle. The fluorescence of W119, the only tryptophan of PYP, is quenched by energy transfer to the chromophore. This depends on the chromophore's transition dipole moment orientation and spectrum, both of which change during the photocycle. The transient fluorescence of W119 thus serves as a sensitive kinetic monitor of the chromophore's structure and orientation and was used for the first time to investigate the photocycle kinetics. From these data and measurements of the ps-fluorescence decay with background illumination (470 nm) we determined the fluorescence lifetimes of W119 in the I(1) and I (1') intermediates. Two coexisting distinct chromophore structures were proposed for the I(1) photointermediate from time-resolved X-ray diffraction ( Ihee, H., et al. Proc. Natl. Acad. Sci. U.S.A., 2005, 102, 7145 ): one with two hydrogen bonds to E46 and Y42, and a second with only one H-bond to Y42 and a different orientation. Only for the first of these is the calculated fluorescence lifetime of 0.22 ns in good agreement with the observed one of 0.26 ns. The second structure has a predicted lifetime of 0.71 ns. Thus, we conclude that in solution only the first I(1) structure occurs. The high resolution structure of the I(1') intermediate, the decay product of I(1) at alkaline pH, is still unknown. We predict from the observed lifetime of 1.3 ns that the chromophore structure of I(1') is quite similar to that of the I(2) intermediate, and I(1') should thus be considered as the alkaline (deprotonated) form of I(2).

The photoactivated PYP domain of Rhodospirillum centenum Ppr accelerates the recovery of the bacteriophytochrome domain after white light illumination.

Ppr from the purple phototrophic bacterium, Rhodospirillum centenum (also known as Rhodocista centenaria), is a hybrid of photoactive yellow protein (PYP), bacteriophytochrome (Bph), and histidine kinase (HK) domains. The holo-Ppr (containing both chromophores) exhibits characteristic absorption maxima at 435 nm due to the PYP domain and at 400, 642, and 701 nm due to the Bph domain. Illumination of the Ppr with white light causes a bleach of both PYP and Bph absorbance; weak blue light primarily bleaches the PYP, and red light activates only the Bph. When excited by blue light, the PYP domain in Ppr recovers with biphasic kinetics at 445 nm (32% with a lifetime of 3.8 min and the remainder with a lifetime of 46 min); white light primarily results in fast recovery, whereas the 130-residue PYP construct shows only the faster kinetics in both blue and white light. Furthermore, there is a slight red shift of the ground state Bph when the PYP is activated; thus, both spectroscopy and kinetics suggest interdomain communication. When Ppr is illuminated with red light, the recovery of the Bph domain to the dark state is significantly slower than that of PYP and is biphasic (57% of the 701 nm decay has a lifetime of 17 min and the remainder a lifetime of 50 min). However, when illuminated with white light or red followed by blue light, the Bph domain in Ppr recovers to the dark-adapted state in a triphasic fashion, where the fastest phase is similar to that of the fast phase of the PYP domain (in white light, 25% of the 701 nm recovery has a lifetime of approximately 1 min) and the slower phases are like the recovery after red light alone. Apo-holo-Ppr (with the biliverdin chromophore only) recovers with biphasic kinetics similar to those of the slower phases of holo-Ppr when activated by either red or white light. We conclude that the photoactivated PYP domain in Ppr accelerates recovery of the activated Bph domain. Phytochromes can be reversibly switched between Pr and Pfr forms by red and far-red light, but the consequence of a bleaching phytochrome is that it cannot be photoreversed by far-red light. We thus postulate that the function of the PYP domain in Ppr is to act as a blue light switch to reverse the effects of red light on the Bph.

Role of a conserved salt bridge between the PAS core and the N-terminal domain in the activation of the photoreceptor photoactive yellow protein.

The effect of ionic strength on the conformational equilibrium between the I(2) intermediate and the signaling state I(2)' of the photoreceptor PYP and on the rate of recovery to the dark state were investigated by time-resolved absorption and fluorescence spectroscopy. With increasing salt concentration up to approximately 600 mM, the recovery rate k(3) decreases and the I(2)/I(2)' equilibrium (K) shifts in the direction of I(2)'. At higher ionic strength both effects reverse. Experiments with mono-(KCl, NaBr) and divalent (MgCl(2), MgSO(4)) salts show that the low salt effect depends on the ionic strength and not on the cation or anion species. These observations can be described over the entire ionic strength range by considering the activity coefficients of an interdomain salt bridge. At low ionic strength the activity coefficient decreases due to counterion screening whereas at high ionic strength binding of water by the salt leads to an increase in the activity coefficient. From the initial slopes of the plots of log k(3) and log K versus the square root of the ionic strength, the product of the charges of the interacting groups was found to be -1.3 +/- 0.2, suggesting a monovalent ion pair. The conserved salt bridge K110/E12 connecting the beta-sheet of the PAS core and the N-terminal domain is a prime candidate for this ion pair. To test this hypothesis, the mutants K110A and E12A were prepared. In K110A the salt dependence of the I(2)/I(2)' equilibrium was eliminated and of the recovery rate was greatly reduced below approximately 600 mM. Moreover, at low salt the recovery rate was six times slower than in wild-type. In E12A significant salt dependence remained, which is attributed to the formation of a novel salt bridge between K110 and E9. At high salt reversal occurs in both mutants suggesting that salting out stabilizes the more compact I(2) structure. However, chaotropic anions like SCN shift the I(2)/I(2)' equilibrium toward the partially unfolded I(2)' form. The salt linkage K110/E12 stabilizes the photoreceptor in the inactive state in the dark and is broken in the light-induced formation of the signaling state, allowing the N-terminal domain to detach from the beta-scaffold PAS core.

Structural role of tyrosine 98 in photoactive yellow protein: effects on fluorescence, gateway, and photocycle recovery.

We have recently shown that the Y98Q mutant of PYP has a major effect on the photocycle kinetics ( approximately 40 times slower recovery). We have now determined the crystal structure of Y98Q at 2.2 A resolution to reveal the role of residue Y98 in the PYP photocycle. Although the overall structure is very similar to that of WT, we observed two major effects of the mutation. One obvious consequence is a conformational change of the beta4-beta5 loop, which includes a repositioning of residue M100. It had previously been shown that the photocycle is slowed by as much as 3 orders of magnitude when residue M100 is substituted or when the conformation is altered as in Rhodocista centenaria PYP. To investigate whether the altered photocycle of Y98Q is due to this repositioning of M100 or is caused by an effect unrelated to M100, we determined the dark recovery kinetics of the Y98Q/M100A mutant. We find the recovery kinetics to be very similar to the M100A single mutant kinetics and therefore conclude that the slower recovery kinetics in Y98Q are most likely due to repositioning of M100. In addition, we find that other substitutions at position 98 (Y98W, Y98L, and Y98A) have differing effects on the photocycle recovery, presumably due to a variable distortion of the beta4-beta5 loop. The second effect of the Y98Q mutation is a repositioning of R52, which is thought to interact with Y98 in WT PYP and now forms new interactions with residues Q99 and Q56. To determine the role of R52, we also characterized an R52A/M100A double mutant and found that the effects on the recovery kinetics ( approximately 2000 slower recovery than WT) are due to unrelated events in the photocycle. Since the Y98Q/M100A recovery kinetics are more similar to those of M100 than R52A/M100A, we conclude that the repositioning of R52, caused by the Y98Q mutation, does not affect the dark state recovery. In addition, it has been proposed that Y98 and P68 are "gateway residues" between which the chromophore must pass during isomerization. We tested the recovery kinetics of mutant P68A and found that, although the gateway may be important for photocycle initiation, its role in recovery to the ground state is minimal.

Properties of the dark and signaling states of photoactive yellow protein probed by solution phase hydrogen/deuterium exchange and mass spectrometry.

The perturbations on conversion from the dark state to the signaling state in photoactive yellow protein have been determined by solution-phase hydrogen/deuterium exchange and mass spectrometry. Both the wild type and M100A mutant are used in this study, with the mutant providing over 90% conversion to the bleached state under steady-state illumination. We found perturbations in both the wild type and the mutant on illumination, consistent with a more flexible structure in the long-lived signaling (I2') state. In the case of the wild type, the conformational changes detected are mainly around the chromophore region. With the M100A mutant, differences in H/D exchange between the light and dark are more extensive as compared to wild type; not only are the chromophore surroundings affected, but significant increases in deuterium uptake in the N-terminus and central beta-sheet are observed as well. On the basis of the data obtained from this study and previous findings, a sequence of events that leads to the perturbation of PYP following chromophore photoisomerization is proposed.

Local stability of Rhodobacter capsulatus cytochrome c2 probed by solution phase hydrogen/deuterium exchange and mass spectrometry.

The hydrogen/deuterium exchange kinetics of Rhodobacter capsulatus cytochrome c2 have been determined using mass spectrometry. As expected, the relative domain stability was generally similar to that of the cytochrome c2 structural homolog, horse heart cytochrome c, but we were able to find evidence to support the presence of a second, small beta-sheet not found in the horse cytochrome, which stabilizes a structural region dominated by Omega loops. Importantly, we find that the so-called hinge region, comprised of 15 amino acids, which include the methionine sixth heme ligand (M96), is destabilized on oxidation, and this destabilization is propagated to a portion of the second Omega loop, most likely through perturbation of two hydrogen bonds that couple these two domains in the three dimensional structure. The mutation of a lysine at position 93 to proline amplifies the destabilization observed on oxidation of the wild-type cytochrome c2 and results in further destabilization observed in regions 52-60, 75-82, and 83-97. This suggests that hydrogen bond interactions involving two bound waters, the T94 hydroxyl, the front heme propionate and the Y75 hydroxyl, are significantly compromised upon mutation. In summary, these observations are consistent with the approximately 20-fold increase in the movement of the hinge away from the heme face in the oxidized cytochrome c2 as determined by ligand binding kinetics. Thus, H/D exchange kinetics can be used to identify relatively subtle structural features and at least in some cases facilitate the understanding of the structural basis of the dynamic properties of proteins.

GHP, a new c-type green heme protein from Halochromatium salexigens and other proteobacteria.

We have isolated a minor soluble green-colored heme protein (GHP) from the purple sulfur bacterium, Halochromatium salexigens, which contains a c-type heme. A similar protein has also been observed in the purple bacteria Allochromatium vinosum and Rhodopseudomonas cryptolactis. This protein has wavelength maxima at 355, 420, and 540 nm and remains unchanged upon addition of sodium dithionite or potassium ferricyanide, indicating either an unusually low or high redox potential, respectively. The amino-acid sequence indicates one heme per peptide chain of 72 residues and reveals weak similarity to the class I cytochromes. The usual sixth heme ligand methionine in these proteins appears to be replaced by a cysteine in GHP. Only one known cytochrome has a cysteine sixth ligand, SoxA (cytochrome c-551) from thiosulfate-oxidizing bacteria, which is low-spin and has a high redox potential because of an un-ionized ligand. The native size of GHP is 34 kDa, its subunit size is 11 kDa, and the net charge is -12, accounting for its very acidic nature. A database search of complete genome sequences reveals six homologs, all hypothetical proteins, from Oceanospirillum sp., Magnetococcus sp., Thiobacillus denitrificans, Dechloromonas aromatica, Thiomicrospira crunogena and Methylobium petroleophilum, with sequence identities of 35-64%. The genetic context is different for each species, although the gene for GHP is transcriptionally linked to several other genes in three out of the six species. These genes, coding for an RNAse, a protease/chaperone, a GTPase, and pterin-4a-carbinolamine dehydratase, appear to be functionally related to stress response and are linked in at least 10 species.

The transient accumulation of the signaling state of photoactive yellow protein is controlled by the external pH.

The signaling state of the photoreceptor photoactive yellow protein is the long-lived intermediate I(2)'. The pH dependence of the equilibrium between the transient photocycle intermediates I(2) and I(2)' was investigated. The formation of I(2)' from I(2) is accompanied by a major conformational change. The kinetics and intermediates of the photocycle and of the photoreversal were measured by transient absorption spectroscopy from pH 4.6 to 8.4. Singular value decomposition (SVD) analysis of the data at pH 7 showed the presence of three spectrally distinguishable species: I(1), I(2), and I(2)'. Their spectra were determined using the extrapolated difference method. I(2) and I(2)' have electronic absorption spectra, with maxima at 370 +/- 5 and 350 +/- 5 nm, respectively. Formation of the signaling state is thus associated with a change in the environment of the protonated chromophore. The time courses of the I(1), I(2), and I(2)' intermediates were determined from the wavelength-dependent transient absorbance changes at each pH, assuming that their spectra are pH-independent. After the formation of I(2)' ( approximately 2 ms), these three intermediates are in equilibrium and decay together to the initial dark state. The equilibrium between I(2) and I(2)' is pH dependent with a pK(a) of 6.4 and with I(2)' the main species above this pK(a). Measurements of the pH dependence of the photoreversal kinetics with a second flash of 355 nm at a delay of 20 ms confirm this pK(a) value. I(2) and I(2)' are photoreversed with reversal times of approximately 55 micros and several hundred microseconds, respectively. The corresponding signal amplitudes are pH dependent with a pK(a) of approximately 6.1. Photoreversal from I(2)' dominates above the pK(a). The transient accumulation of I(2)', the active state of photoactive yellow protein, is thus controlled by the proton concentration. The rate constant k(3) for the recovery to the initial dark state also has a pK(a) of approximately 6.3. This equality of the equilibrium and kinetic pK(a) values is not accidental and suggests that k(3) is proportional to [I(2)'].

Photocycle and photoreversal of photoactive yellow protein at alkaline pH: kinetics, intermediates, and equilibria.

Since the habitat of Halorhodospira halophila is distinctly alkaline, we investigated the kinetics and intermediates of the photocycle and photoreversal of the photoreceptor photoactive yellow protein (PYP) from pH 8 to 11. SVD analysis of the transient absorption time traces in a broad wavelength range (330-510 nm) shows the presence of three spectrally distinct species (I1, I1', and I2') at pH 10. The spectrum of I1' was obtained in two different ways. The maximal absorption is at 425 nm. I1' probably has a deprotonated chromophore and may be regarded as the alkaline form of I2'. At pH 10, the I1 intermediate decays in approximately 330 micros in part to I1' before I1 and I1' decay further to I2' in approximately 1 ms. From the rise of I2' (approximately 1 ms) to the end of the photocycle, the three intermediates (I1, I1', and I2') remain in equilibrium and decay together to P in approximately 830 ms. Assuming that the spectra of I1, I1', and I2' are pH-independent, their time courses were determined. On the millisecond to second time scale, they are in a pH-dependent equilibrium with a pKa of approximately 9.9. With an increase in pH, the I1 and I1' populations increase at the expense of the amount of I2'. The apparent rate constant for the recovery of P slows with an increase in pH with a pKa of approximately 9.7. The equal pH dependence of this rate and the equilibrium concentrations follows, if we assume that the equilibration rates between the intermediates are much faster than the recovery rate and that the recovery occurs from I2'. The pKa of approximately 9.9 is assigned to the deprotonation of the phenol of the surface-exposed chromophore in the I1'-I2' equilibrium. The I1-I1' equilibrium is pH-independent. Photoreversal experiments at pH 10 with the second flash at 355 nm indicate the presence of only one I2-like intermediate, which we assign on the basis of its lambda(max) value to I2'. After the rapid unresolved photoisomerization to I2'(trans), the reversal pathway back to P involves two sequential steps (60 micros and 3 ms). The amplitude spectra show that I1'(trans) and I1(trans) intermediates participate in this reversal.

Structural evolution of the chromophore in the primary stages of trans/cis isomerization in photoactive yellow protein.

We have studied the structural changes induced by optical excitation of the chromophore in wild-type photoactive yellow protein (PYP) in liquid solution with a combined approach of polarization-sensitive ultrafast infrared spectroscopy and density functional theory calculations. We identify the nuC8-C9 marker modes for solution phase PYP in the P and I0 states, from which we derive that the first intermediate state I0 that appears with a 3 ps time constant can be characterized to have a cis geometry. This is the first unequivocal demonstration that the formation of I0 correlates with the conversion from the trans to the cis state. For the P and I0 states we compare the experimentally measured vibrational band patterns and anisotropies with calculations and find that for both trans and cis configurations the planarity of the chromophore has a strong influence. The C7=C8-(C9=O)-S moiety of the chromophore in the dark P state has a trans geometry with the C=O group slightly tilted out-of-plane, in accordance with the earlier reported structure obtained in an X-ray diffraction study of PYP crystals. In the case of I0, experiment and theory are only in agreement when the C7=C8-(C9=O)-S moiety has a planar configuration. We find that the carboxylic side group of Glu46 that is hydrogen-bonded to the chromophore phenolate oxygen does not alter its orientation on going from the electronic ground P state, via the electronic excited P state to the intermediate I0 state, providing conclusive experimental evidence that the primary stages of PYP photoisomerization involve flipping of the enone thioester linkage without significant relocation of the phenolate moiety.

Time-resolved single tryptophan fluorescence in photoactive yellow protein monitors changes in the chromophore structure during the photocycle via energy transfer.

We show from time-resolved fluorescence intensity and depolarization experiments that the fluorescence of the unique tryptophan W119 of PYP is quenched by energy transfer to the 4-hydroxycinnamoyl chromophore. Whereas the intensity decay has a time constant of 0.18 ns in P, the decay in the absence of the cofactor (apo-PYP) has a single exponential lifetime of 4.8 ns. This difference in lifetime with and without acceptor can be explained quantitatively on the basis of energy transfer and the high-resolution X-ray structure of P, which allows an accurate calculation of the kappa2 factor. Fluorescence depolarization experiments with donor and acceptor indicate that both are immobilized so that kappa2 is constant on the fluorescence time scale. Using background illumination from an LED emitting at 470 nm, we measured the time-resolved fluorescence in a photostationary mixture of P and the intermediates I2 and I2'. The composition of the photostationary mixture depends on pH and changes from mainly I2 at low pH to predominantly I2' at high pH. The I2/I2' equilibrium is pH-dependent with a pKa of approximately 6.3. In I2 the lifetime increases to approximately 0.82 ns. This is not due to a change in distance or to the increase in spectral overlap but is primarily a consequence of a large decrease in kappa2. Kappa2 was calculated from the available X-ray structures and decreases from approximately 2.7 in P to 0.27 in I2. This change in kappa2 is caused by the isomerization of the acceptor, which leads to a reorientation of its transition dipole moment. We have here a rare case of the kappa2 factor dominating the change in energy transfer. The fluorescence decay in the light is pH-dependent. From an SVD analysis of the light/dark difference intensity decay at a number of pH values, we identify three species with associated lifetimes: P (0.18 ns), I2 (0.82 ns), and X (0.04 ns). On the basis of the pH dependence of the amplitudes associated with I2 and X, with a pKa of approximately 6.3, we assign the third species to the signaling state I2'. The absorption spectra of the 0.82 and 0.04 ns species were calculated from the pH dependence of their fluorescence amplitudes and of the photostationary light/dark difference absorption spectra. The lambda(max) values of these spectra (372 and 352 nm) identify the 0.82 and 0.04 ns components with I2 and I2', respectively, and validate the fluorescence data analysis. The mutant E46Q allows a further test of the energy transfer explanation, since lowering the pH in the dark leads to a bleached state with an increased spectral overlap but without the isomerization-induced decrease in kappa2. The measured lifetime of 0.04 ns is in excellent agreement with predictions based on energy transfer and the X-ray structure.

Effect of salt and pH on the activation of photoactive yellow protein and gateway mutants Y98Q and Y98F.

We investigated the photocycle of mutants Y98Q and Y98F of the photoactive yellow protein (PYP) from Halorhodospira halophila. Y98 is located in the beta4-beta5 loop and is thought to interact with R52 in the alpha3-alpha4 loop thereby stabilizing this region. Y98 is conserved in all known PYP species, except in Ppr and Ppd where it is replaced by F. We find that replacement of Y98 by F has no significant effect on the photocycle kinetics. However, major changes were observed with the Y98Q mutant. Our results indicate a requirement for an aromatic ring at position 98, especially for recovery and a normal I1/I2 equilibrium. The ring of Y98 could stabilize the beta4-beta5 loop. Alternatively, the Y98 ring could transiently interact with the isomerized chromophore ring, thereby stabilizing the I2 intermediate in the I1/I2 equilibrium. For Y98Q, the decay of the signaling state I2' was slowed by a factor of approximately 40, and the rise of the I2 and I2' intermediates was slowed by a factor of 2-3. Moreover, the I1 intermediate is in a pH-dependent equilibrium with I2/I2' with the ratio of the I1 and I2 populations close to one at pH 7 and 50 mM KCl. From pH 5.5 to 8, the equilibrium shifts toward I1, with a pKa of approximately 6.3. Above pH 8, the populations of I1 and I2/I2' decrease due to an equilibrium between I1 and an additional species I1' which absorbs at approximately 425 nm (pKa approximately 9.8) and which we believe to be an I2-like form with a surface-exposed deprotonated chromophore. The I1/I2/I2' equilibrium was found to be strongly dependent on the KCl concentration, with salt stabilizing the signaling state I2' up to 600 mM KCl. This salt-induced transition to I2' was analyzed and interpreted as ion binding to a specific site. Moreover, from analysis of the amplitude spectra, we conclude that KCl exerts its major effect on the I2 to I2' transition, i.e., the global conformational change leading to the signaling state I2' and the exposure of a hydrophobic surface patch. In wild type and Y98F, the I1/I2 equilibrium is more on the side of I2/I2' as compared to Y98Q but is also salt-dependent at pH 7. The I2 to I2' transition appears to be controlled by an ionic lock, possibly involving the salt bridge between K110 on the beta-scaffold and E12 on the N-terminal cap. Salt binding would break the salt bridge and weaken the interaction between the two domains, facilitating the release of the N-terminal domain from the beta-scaffold in the formation of I2'.

Thermochromatium tepidum photoactive yellow protein/bacteriophytochrome/diguanylate cyclase: characterization of the PYP domain.

The purple phototrophic bacterium, Thermochromatium tepidum, contains a gene for a chimeric photoactive yellow protein/bacteriophytochrome/diguanylate cyclase (Ppd). We produced the Tc. tepidum PYP domain (Tt PYP) in Escherichia coli, and found that it has a wavelength maximum at 358 nm due to a Leu46 substitution of the color-tuning Glu46 found in the prototypic Halorhodospira halophila PYP (Hh PYP). However, the 358 nm dark-adapted state is in a pH-dependent equilibrium with a yellow species absorbing at 465 nm (pK(a) = 10.2). Following illumination at 358 nm, photocycle kinetics are characterized at pH 7.0 by a small bleach and red shift to what appears to be a long-lived cis intermediate (comparable to the I(2) intermediate in Hh PYP). The recovery to the dark-adapted state has a lifetime of approximately 4 min, which is approximately 1500 times slower than that for Hh PYP. However, when the Tt PYP is illuminated at pH values above 7.5, the light-induced difference spectrum indicates a pH-dependent equilibrium between the I(2) intermediate and a red-shifted 440 nm intermediate. This equilibrium could be responsible for the sigmoidal pH dependence of the recovery of the dark-adapted state (pK(a) = 8.8). In addition, the light-induced difference spectrum shows that, at pH values above 9.3, there is an apparent bleach near 490 nm superimposed on the 358 and 440 nm changes, which we ascribe to the equilibrium between the protonated and ionized dark-adapted forms. The L46E mutant of Tt PYP has a wavelength maximum at 446 nm, resembling wild-type Hh PYP. The kinetics of recovery of L46E following illumination with white light are slow (lifetime of 15 min at pH 7), but are comparable to those of wild-type Tt PYP. We conclude that Tt PYP is unique among the PYPs studied to date in that it has a photocycle initiated from a dark-adapted state with a protonated chromophore at physiological pH. However, it is kinetically most similar to Rhodocista centenaria PYP (Ppr) despite the very different absorption spectra due to the lack of E46.

Photoreversal kinetics of the I1 and I2 intermediates in the photocycle of photoactive yellow protein by double flash experiments with variable time delay.

We investigated the kinetics of photoreversal from the I(1) and I(2) intermediates of photoactive yellow protein (PYP) by time-resolved optical absorption spectroscopy with double flash excitation. A first flash, at 430 nm, initiated the photocycle. After a variable time delay, the I(1) intermediate was photoreversed by a second flash, at 500 nm, or a mixture of I(2) and I(2)' intermediates was photoreversed by a second flash, at 355 nm. By varying the delay from 1 micros to 3 s, we were able to selectively excite the intermediates I(1), I(2), and I(2)'. The photoreversal kinetics of I(2) and I(2)' at 21 different delays and two wavelengths (340 and 450 nm) required two exponentials for a global fit with time constants of tau(1) = 57 +/- 5 micros and tau(2) = 380 +/- 40 micros (pH 6, 20 degrees C). These were assigned to photoreversal from sequential I(2) and I(2)' intermediates, respectively. The good agreement of the delay dependence of the two amplitudes, A(1) and A(2), with the time dependence of the I(2) and I(2)' populations provided strong evidence for the sequential model. The persistence of A(1) beyond delay times of 5 ms and its decay, together with A(2) around 500 ms, suggest moreover that I(2) and I(2)' are in thermal equilibrium. The wavelength dependence of the photoreversal kinetics was measured at 26 wavelengths from 510 to 330 nm at the two fixed delays of 1 and 10 ms. These data also required two exponentials for a global fit with tau(1) = 59 +/- 5 micros and tau(2) = 400 +/- 40 micros, in good agreement with the delay results. Photoreversal from I(2)' is slower than from I(2), since, in addition to chromophore protonation, the global conformational change has to be reversed. Our data thus provide a first estimate of about 59 micros for deprotonation and 400 micros for the structural change, which also occurs in the thermal decay of the signaling state but is obscured there since reisomerization is rate-limiting. The first step in photoreversal is rapid cis-trans isomerization of the chromophore, which we could not resolve, but which was detected by the instantaneous increase in absorbance between 330 and 380 nm. In agreement with this observation, the spectrum of the I(2)'(trans) intermediate, derived from the A(2) amplitude spectrum, has a much larger extinction coefficient than the spectrum of the I(2)'(cis) intermediate. With a first flash, at 430 nm, and a second flash, at 500 nm, we observed efficient photoreversal of the I(1) intermediate at a delay of 20 micros when most molecules in the cycle are in I(1). We conclude that each of the three intermediates studied can be reversed by a laser flash. Depending on the progression of the photocycle, reversal becomes slower with the time delay, thus mirroring the individual steps of the forward photocycle.