Molecular dynamics simulations of photoactive yellow protein (PYP) in three states of its photocycle: a comparison with X-ray and NMR data and analysis of the effects of Glu46 deprotonation and mutation

Photoactive yellow protein (PYP) is a prototype of the PAS domain superfamily of signaling proteins. The signaling process is coupled to a three-state photocycle. After the photoinduced trans-cis isomerization of the chromophore, 4-hydroxycinnamic acid (pCA), an early intermediate (pR) is formed, which proceeds to a second intermediate state (pB) on a sub-millisecond time scale. The signaling process is thought to be connected to the conformational changes upon the formation of pB and its recovery to the ground state (pG), but the exact signaling mechanism is not known. Experimental studies of PYP by solution NMR and X-ray crystallography suggest a very flexible protein backbone in the ground as well as in the signaling state. The relaxation from the pR to the pB state is accompanied by the protonation of the chromophore's phenoxyl group. This was found to be of crucial importance for the relaxation process. With the goal of gaining a better understanding of these experimental observations on an atomistic level, we performed five MD simulations on the three different states of PYP: a 1 ns simulation of PYP in its ground state [pG(MD)], a 1 ns simulation of the pR state [pR(MD)], a 2 ns simulation of the pR state with the chromophore protonated (pRprot), a 2 ns simulation of the pR state with Glu46 exchanged by Gln (pRGln) and a 2 ns simulation of PYP in its signaling state [pB(MD)]. Comparison of the pG simulation results with X-ray and NMR data, and with the results obtained for the pB simulation, confirmed the experimental observations of a rather flexible protein backbone and conformational changes during the recovery of the pG from the pB state. The conformational changes in the region around the chromophore pocket in the pR state were found to be crucially dependent on the strength of the Glu46-pCA hydrogen bond, which restricts the mobility of the chromophore in its unprotonated form considerably. Both the mutation of Glu46 with Gln and the protonation of the chromophore weaken this hydrogen bond, leading to an increased mobility of pCA and large structural changes in its surroundings. These changes, however, differ considerably during the pRGln and pRprot simulations, providing an atomistic explanation for the enhancement of the rate constant in the Gln46 mutant. Electronic supplementary material to this article is available at and is accessible for athorized users. Electronic Publication     

Lack of negative charge in the E46Q mutant of photoactive yellow protein prevents partial unfolding of the blue-shifted intermediate

The long-lived light-induced intermediate (pB) of the E46Q mutant (glutamic acid is replaced by glutamine at position 46) of photoactive yellow protein (PYP) has been investigated by NMR spectroscopy. The ground state of this mutant is very similar to that of wild-type PYP (WT), whereas the pB state, formed upon illumination, appears to be much more structured in E46Q than in WT. The differences are most striking in the N-terminal domain of the protein. In WT, the side-chain carboxylic group of E46 is known to donate its proton to the chromophore upon illumination. The absence of the carboxylic group near the chromophore in the E46Q mutant prohibits the formation of a negative charge at this position upon formation of pB. This prevents the partial unfolding of the mutant, as evidenced from NMR chemical shift comparison and proton/deuterium (H/D) exchange studies.     

Transient exposure of hydrophobic surface in the photoactive yellow protein monitored with Nile Red

In this study we have investigated binding of the fluorescent hydrophobicity probe Nile Red to the photoactive yellow protein (PYP), to characterize the exposure and accessibility of hydrophobic surface upon formation of the signaling state of this photoreceptor protein. Binding of Nile Red, reflected by a large blue shift and increase in fluorescence quantum yield of the Nile Red emission, is observed exclusively when PYP resides in its signaling state. N-terminal truncation of the protein allows assignment of the region surrounding the chromophore as the site where Nile Red binds to PYP. We also observed a pH dependence of the affinity of Nile Red for pB, which we propose is caused by pH dependent differences of the structure of the signaling state. From a comparative analysis of the kinetics of Nile Red binding and transient absorption changes in the visible region we can conclude that protonation of the chromophore precedes the exposure of a hydrophobic surface near the chromophore binding site, upon formation of the signaling state. Furthermore, the data presented here favor the view that the signaling state is structurally heterogeneous.     

pH Dependence of the photocycle kinetics of the E46Q mutant of photoactive yellow protein: protonation equilibrium between I1 and I2 intermediates,chromophore deprotonation by hydroxyl uptake,and protonation relaxation of the dark state

The kinetics of the photocycle of PYP and its mutants E46Q and E46A were investigated as a function of pH. E46 is the putative donor of the chromophore which becomes protonated in the I(2) intermediate. For E46Q we find that I(2) is in a pH-dependent equilibrium with its precursor I(1)' with a pK(a) of 8.15 and n = 1. From this result and from experiments with pH indicator dyes, we conclude that in the I(1)' to I(2) transition one proton is taken up from the external medium. The pK(a) of 8.15 is that of the surface-exposed chromophore in the equilibrium between I(1)' and I(2) and is close to that of the phenolate group of p-hydroxycinnamic acid. The pH-dependent I(1)'/I(2) equilibrium with associated H(+) uptake is reminiscent of the M(I)/M(II) equilibrium in the formation of the signaling state of rhodopsin. Well above this pK(a) no I(2) is formed and I(1)' returns in a pH-independent manner to the initial state P. The decay rate for the return to P via I(2) is between pH 4 and pH 8, exactly proportional to the hydroxide concentration (first order), and the deprotonation of the chromophore in this transition occurs by hydroxide uptake. Well above the pK(a) of 8.15 the apparent rate constant for the return to P is constant due to the branching from I(1)'. Complementary measurements with the pH indicator dye cresol red at pH 8.3 show that the remaining PYP molecules that still cycle via I(2) take up one proton in the formation of I(2). Together, these observations provide compelling evidence that during the photocycle the chromophore in E46Q is protonated and deprotonated from the external medium. For the yellow form of the mutant E46A the apparent rate constant for the return to P is also linear in [OH(-)] below about pH 8.3 and constant above about pH 9.5, with a pK(a) value of 8.8 for I(1)', suggesting a similar mechanism of chromophore protonation/deprotonation as in E46Q. For wild type qualitatively similar observations were made: the amplitude of I(2) decreased at alkaline pH, I(1)' and I(2) were in equilibrium, and I(1)' decayed together with the return to P. Chromophore hydrolysis prevented, however, an accurate determination of the pK(a) of I(1)'. We estimate that its value is above 11. The ground state P is in the dark in a pH-dependent equilibrium with a low-pH bleached form P(bl) with protonated chromophore. The pK(a) values for these equilibria are 4.8 and 7.9 for E46Q and E46A, respectively. When the pH is close to these pK(a)'s, the kinetics of the photocycle contains additional components in the millisecond time range. Using pH-jump stopped-flow experiments, we show that these contributions are due to the relaxation of the P/P(bl) equilibrium which is perturbed by the rapid decrease in the P concentration caused by the flash excitation of P. The condition for the occurrence of this effect is that the relaxation time of the P/P(bl) equilibrium is faster than the photocycle time.     

Kinetics of proton uptake and dye binding by photoactive yellow protein in wild type and in the E46Q and E46A mutants

We studied the kinetics of proton uptake and release by photoactive yellow protein (PYP) from Ectothiorhodospira halophila in wild type and the E46Q and E46A mutants by transient absorption spectroscopy with the pH-indicator dyes bromocresol purple or cresol red in unbuffered solution. In parallel, we investigated the kinetics of chromophore protonation as monitored by the rise and decay of the blue-shifted state I(2) (lambda(max) = 355 nm). For wild type the proton uptake kinetics is synchronized with the fast phase of I(2) formation (tau = 500 micros at pH 6.2). The transient absorption signal from the dye also contains a slower component which is not due to dye deprotonation but is caused by dye binding to a hydrophobic patch that is transiently exposed in the structurally changed and partially unfolded I(2) intermediate. This conclusion is based on the wavelength, pH, and concentration dependence of the dye signal and on dye measurements in the presence of buffer. SVD analysis, moreover, indicates the presence of two components in the dye signal: protonation and dye binding. The dye binding has a rise time of about 4 ms and is coupled kinetically with a transition between two I(2) intermediates. In the mutant E46Q, which lacks the putative internal proton donor E46, the formation of I(2) is accelerated, but the proton uptake kinetics remains kinetically coupled to the fast phase of I(2) formation (tau = 100 micros at pH 6.3). For this mutant the protein conformational change, as monitored by the dye binding, occurs with about the same time constant as in wild type but with reduced amplitude. In the alkaline form of the mutant E46A the formation of the I(2)-like intermediate is even faster as is the proton uptake (tau = 20 micros at pH 8.3). No dye binding occurred in E46A, suggesting the absence of a conformational change. In all of the systems proton release is synchronized with the decay of I(2). Our results support mechanisms in which the chromophore of PYP is protonated directly from the external medium rather than by the internal donor E46.     

pH dependence of the photoactive yellow protein photocycle investigated by time-resolved crystallography

Visualizing the three-dimensional structures of a protein during its biological activity is key to understanding its mechanism. In general, protein structure and function are pH-dependent. Changing the pH provides new insights into the mechanisms that are involved in protein activity. Photoactive yellow protein (PYP) is a signaling protein that serves as an ideal model for time-dependent studies on light-activated proteins. Its photocycle is studied extensively under different pH conditions. However, the structures of the intermediates remain unknown until time-resolved crystallography is employed. With the newest beamline developments, a comprehensive time series of Laue data can now be collected from a single protein crystal. This allows us to vary the pH. Here we present the first structure, to our knowledge, of a short-lived protein-inhibitor complex formed in the pB state of the PYP photocycle at pH 4. A water molecule that is transiently stabilized in the chromophore active site prevents the relaxation of the chromophore back to the trans configuration. As a result, the dark-state recovery is slowed down dramatically. At pH 9, PYP stops cycling through the pB state altogether. The electrostatic environment in the chromophore-binding site is the likely reason for this altered kinetics at different pH values.     

Predicting the signaling state of photoactive yellow protein

As a bacterial blue light sensor the photoactive yellow protein (PYP) undergoes conformational changes upon signal transduction. The absorption of a photon triggers a series of events that are initially localized around the protein chromophore, extends to encompass the whole protein within microseconds, and leads to the formation of the transient pB signaling state. We study the formation of this signaling state pB by molecular simulation and predict its solution structure. Conventional straightforward molecular dynamics is not able to address this formation process due to the long (microsecond) timescales involved, which are (partially) caused by the presence of free energy barriers between the metastable states. To overcome these barriers, we employed the parallel tempering (or replica exchange) method, thus enabling us to predict qualitatively the formation of the PYP signaling state pB. In contrast to the receptor state pG of PYP, the characteristics of this predicted pB structure include a wide open chromophore-binding pocket, with the chromophore and Glu(46) fully solvent-exposed. In addition, loss of alpha-helical structure occurs, caused by the opening motion of the chromophore-binding pocket and the disruptive interaction of the negatively charged Glu(46) with the backbone atoms in the hydrophobic core of the N-terminal cap. Recent NMR experiments agree very well with these predictions.     

Protonation states and pH titration in the photocycle of photoactive yellow protein

Photoactive yellow protein (PYP) undergoes a light-driven cycle of color and protonation states that is part of a mechanism of bacterial phototaxis. This article concerns functionally important protonation states of PYP and the interactions that stabilize them, and changes in the protonation state during the photocycle. In particular, the chromophore pK(a) is known to be shifted down so that the chromophore is negatively charged in the ground state (dark state) even though it is buried in the protein, while nearby Glu46 has an unusually high pK(a). The photocycle involves changes of one or both of these protonation states. Calculations of pK(a) values and protonation states using a semi-macroscopic electrostatic model are presented for the wild-type and three mutants, in both the ground state and the bleached (I(2)) intermediate state. Calculations allowing multiple H-bonding arrangements around the chromophore also have been carried out. In addition, ground-state pK(a) values of the chromophore have been measured by UV-visible spectroscopy for the wild-type and the same three mutants. Because of the unusual protonation states and strong electrostatic interactions, PYP represents a severe test of the ability of theoretical models to yield correct calculations of electrostatic interactions in proteins. Good agreement between experiment and theory can be obtained for the ground state provided the protein interior is assumed to have a relatively low dielectric constant, but only partial agreement between theory and experiment is obtained for the bleached state. We also present a reinterpretation of previously published data on the pH-dependence of the recovery of the ground state from the bleached state. The new analysis implies a pK(a) value of 6.37 for Glu46 in the bleached state, which is consistent with other available experimental data, including data that only became available after this analysis. The new analysis suggests that signal transduction is modulated by the titration properties of the bleached state, which are in turn determined by electrostatic interactions. Overall, the results of this study provide a quantitative picture of the interactions responsible for the unusual protonation states of the chromophore and Glu46, and of protonation changes upon bleaching.     

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.     

Kinetics of and intermediates in a photocycle branching reaction of the photoactive yellow protein from Ectothiorhodospira halophila.

We have studied the kinetics of the blue light-induced branching reaction in the photocycle of photoactive yellow protein (PYP) from Ectothiorhodospira halophila, by nanosecond time-resolved UV/Vis spectroscopy. As compared to the parallel dark recovery reaction of the presumed blue-shifted signaling state pB, the light-induced branching reaction showed a 1000-fold higher rate. In addition, a new intermediate was detected in this branching pathway, which, compared to pB, showed a larger extinction coefficient and a blue-shifted absorption maximum. This substantiates the conclusion that isomerization of the chromophore is the rate-controlling step in the thermal photocycle reactions of PYP and implies that absorption of a blue photon leads to cis-->trans isomerization of the 4-hydroxy-cinnamyl chromophore of PYP in its pB state.     

Titration of aspartate-85 in bacteriorhodopsin: what it says about chromophore isomerization and proton release.

Titration of Asp-85, the proton acceptor and part of the counterion in bacteriorhodopsin, over a wide pH range (2-11) leads us to the following conclusions: 1) Asp-85 has a complex titration curve with two values of pKa; in addition to a main transition with pKa = 2.6 it shows a second inflection point at high pH (pKa = 9.7 in 150-mM KCl). This complex titration behavior of Asp-85 is explained by interaction of Asp-85 with an ionizable residue X'. As follows from the fit of the titration curve of Asp-85, deprotonation of X' increases the proton affinity of Asp-85 by shifting its pKa from 2.6 to 7.5. Conversely, protonation of Asp-85 decreases the pKa of X' by 4.9 units, from 9.7 to 4.8. The interaction between Asp-85 and X' has important implications for the mechanism of proton transfer. In the photocycle after the formation of M intermediate (and protonation of Asp-85) the group X' should release a proton. This deprotonated state of X' would stabilize the protonated state of Asp-85.2) Thermal isomerization of the chromophore (dark adaptation) occurs on transient protonation of Asp-85 and formation of the blue membrane. The latter conclusion is based on the observation that the rate constant of dark adaptation is directly proportional to the fraction of blue membrane (in which Asp-85 is protonated) between pH 2 and 11. The rate constant of isomerization is at least 10(4) times faster in the blue membrane than in the purple membrane. The protonated state of Asp-85 probably is important for the catalysis not only of all-trans <=> 13-cis thermal isomerization during dark adaptation but also of the reisomerization of the chromophore from 13-cis to all-trans configuration during N-->O-->bR transition in the photocycle. This would explain why Asp-85 stays protonated in the N and O intermediates.     

Vibrational spectroscopy of bacteriorhodopsin mutants. Evidence that Thr-46 and Thr-89 form part of a transient network of hydrogen bonds.

The role of Thr-46 and Thr-89 in the bacteriorhodopsin photocycle has been investigated by Fourier transform infrared difference spectroscopy and time-resolved visible absorption spectroscopy of site-directed mutants. Substitutions of Thr-46 and Thr-89 reveal alterations in the chromophore and protein structure during the photocycle, relative to wild-type bacteriorhodopsin. The mutants T89D and to a lesser extent T89A display red shifts in the visible lambda max of the light-adapted states compared with wild type. During the photocycle, T89A exhibits an increased decay rate of the K intermediate, while a K intermediate is not detected in the photocycle of T89D at room temperature. In the carboxyl stretch region of the Fourier transform infrared difference spectra of T89D, a new band appears as early as K formation which is attributed to the deprotonation of Asp-89. Along with this band, an intensity increase occurs in the band assigned to the protonation of Asp-212. In the mutant T46V, a perturbation in the environment of Asp-96 is detected in the L and M intermediates which corresponds to a drop in its pK alpha. These data indicate that Thr-89 is located close to the chromophore, exerts steric constraints on it during all-trans to 13-cis isomerization, and is likely to participate in a hydrogen-bonding network that extends to Asp-212. In addition, a transient interaction between Thr-46 and Asp-96 occurs early in the photocycle. In order to explain these results, a previously proposed model of proton transport is extended to include the existence of a transient network of hydrogen-bonded residues. This model can account for the protonation changes of key amino acid residues during the photocycle of bacteriorhodopsin.     

Proton transfer in the photoreceptors phytochrome and photoactive yellow protein.

Light-induced activation of the photoreceptors phytochrome and photoactive yellow protein (PYP) is accompanied by protonation changes of the respective chromophores and key residues in the protein moiety. For both systems, proton exchange with the external medium could be observed with pH electrode measurements and with UV-visible absorption spectroscopy using appropriate pH indicator dyes. From these signals, the stoichiometry of proton release and uptake, respectively, was determined by different calibration procedures which will be presented and discussed. Kinetic information on these processes is only available from time-resolved measurements with pH indicator dyes. Vibrational spectroscopy methods such as Fourier transform infrared spectroscopy and resonance Raman scattering provided information on the protonation state of individual functional groups suggesting that internal proton transfer processes are involved as well. Deuterium kinetic isotope effects that occurred in the Pr --> Pfr phototransformation of the bacteriophytochromes Cph1 and Agp1 were consistent with proton transfer reactions as rate-limiting steps. In contrast, the apparent rate constants in the photocycle of PYP exhibited only small kinetic isotope effects that could not be interpreted conclusively. Possible mechanisms of proton transfer in the activation of phytochrome and PYP will be discussed.     

Comprehensive determination of protein tyrosine pKa values for photoactive yellow protein using indirect 13C NMR spectroscopy

Upon blue-light irradiation, the bacterium Halorhodospira halophila is able to modulate the activity of its flagellar motor and thereby evade potentially harmful UV radiation. The 14 kDa soluble cytosolic photoactive yellow protein (PYP) is believed to be the primary mediator of this photophobic response, and yields a UV/Vis absorption spectrum that closely matches the bacterium's motility spectrum. In the electronic ground state, the para-coumaric acid (pCA) chromophore of PYP is negatively charged and forms two short hydrogen bonds to the side chains of Glu-46 and Tyr-42. The resulting acid triad is central to the marked pH dependence of the optical-absorption relaxation kinetics of PYP. Here, we describe an NMR approach to sequence-specifically follow all tyrosine side-chain protonation states in PYP from pH 3.41 to 11.24. The indirect observation of the nonprotonated ¹³C_γ resonances in sensitive and well-resolved two-dimensional ¹³C-¹H spectra proved to be pivotal in this effort, as observation of other ring-system resonances was hampered by spectral congestion and line-broadening due to ring flips. We observe three classes of tyrosine residues in PYP that exhibit very different pK_a values depending on whether the phenolic side chain is solvent-exposed, buried, or hydrogen-bonded. In particular, our data show that Tyr-42 remains fully protonated in the pH range of 3.41–11.24, and that pH-induced changes observed in the photocycle kinetics of PYP cannot be caused by changes in the charge state of Tyr-42. It is therefore very unlikely that the pCA chromophore undergoes changes in its electrostatic interactions in the electronic ground state.     

Dynamics of protein and chromophore structural changes in the photocycle of photoactive yellow protein monitored by time-resolved optical rotatory dispersion

The dynamics of the PYP photocycle have been studied using time-resolved optical rotatory dispersion (TRORD) spectroscopy in the visible and far-UV spectral regions to probe the changes in the chromophore configuration and the protein secondary structure, respectively. The changes in the secondary structure in PYP upon photoisomerization of the chromophore can be described by two exponential lifetimes of 2 +/- 0.8 and 650 +/- 100 ms that correspond to unfolding and refolding processes, respectively. The TRORD experiments that follow the dynamics of the chromophore report three exponential components, with lifetimes of 10 +/- 3 micros, 1.5 +/- 0.5 ms, and 515 +/- 110 ms. A comparison of the kinetic behaviors of the chromophore and protein shows that during the decay of pR(465) an initial relaxation that is localized to the chromophore hydrophobic pocket precedes the formation of the chromophore and protein structures found in pB(355). In contrast, the protein and chromophore processes occur with similar time constants during inactivation of the signaling state.     

Deuterium Isotope Effects in the Photocycle Transitions of the Photoactive Yellow Protein

The Photoactive Yellow Protein (PYP) from Halorhodospira halophila (formerly Ectothiorhodospira halophila) is increasingly used as a model system. As such, a thorough understanding of the photocycle of PYP is essential. In this study we have combined information from pOH- (or pH-) dependence and (kinetic) deuterium isotope effects to elaborate on existing photocycle models. For several characteristics of PYP we were able to make a distinction between pH- and pOH-dependence, a nontrivial distinction when comparing data from samples dissolved in H₂O and D₂O. It turns out that most characteristics of PYP are pOH-dependent. We confirmed the existence of a pB′ intermediate in the pR to pB transition of the photocycle. In addition, we were able to show that the pR to pB′ transition is reversible, which explains the previously observed biexponential character of the pR-to-pB photocycle step. Also, the absorption spectrum of pB′ is slightly red-shifted with respect to pB. The recovery of the pG state is accompanied by an inverse kinetic deuterium isotope effect. Our interpretation of this is that before the chromophore can be isomerized, it is deprotonated by a hydroxide ion from solution. From this we propose a new photocycle intermediate, pB^deprot, from which pG is recovered and which is in equilibrium with pB. This is supported in our data through the combination of the observed pOH and pH dependence, together with the kinetic deuterium isotope effect.     

Dual photoactive species in Glu46Asp and Glu46Ala mutants of photoactive yellow protein: a pH-driven color transition.

Photoactive yellow protein (PYP) is a blue light sensor present in the purple photosynthetic bacterium Ectothiorhodospira halophila, which undergoes a cyclic series of absorbance changes upon illumination at its lambda(max) of 446 nm. The anionic p-hydroxycinnamoyl chromophore of PYP is covalently bound as a thiol ester to Cys69, buried in a hydrophobic pocket, and hydrogen-bonded via its phenolate oxygen to Glu46 and Tyr42. The chromophore becomes protonated in the photobleached state (I(2)) after it undergoes trans-cis isomerization, which results in breaking of the H-bond between Glu46 and the chromophore and partial exposure of the phenolic ring to the solvent. In previous mutagenesis studies of a Glu46Gln mutant, we have shown that a key factor in controlling the color and photocycle kinetics of PYP is this H-bonding system. To further investigate this, we have now characterized Glu46Asp and Glu46Ala mutants. The ground-state absorption spectrum of the Glu46Asp mutant shows a pH-dependent equilibrium (pK = 8.6) between two species: a protonated (acidic) form (lambda(max) = 345 nm), and a slightly blue-shifted deprotonated (basic) form (lambda(max) = 444 nm). Both of these species are photoactive. A similar transition was also observed for the Glu46Ala mutant (pK = 7.9), resulting in two photoactive red-shifted forms: a basic species (lambda(max) = 465 nm) and a protonated species (lambda(max) = 365 nm). We attribute these spectral transitions to protonation/deprotonation of the phenolate oxygen of the chromophore. This is demonstrated by FT Raman spectra. Dark recovery kinetics (return to the unphotolyzed state) were found to vary appreciably between these various photoactive species. These spectral and kinetic properties indicate that the hydrogen bond between Glu46 and the chromophore hydroxyl group is a dominant factor in controlling the pK values of the chromophore and the glutamate carboxyl.     

Resonance Raman spectroscopy and quantum chemical calculations reveal structural changes in the active site of photoactive yellow protein

Photoactive yellow protein (PYP) is a bacterial photoreceptor containing a 4-hydroxycinnamyl chromophore. Photoexcitation of PYP triggers a photocycle that involves at least two intermediate states: an early red-shifted PYP(L) intermediate and a long-lived blue-shifted PYP(M) intermediate. In this study, we have explored the active site structures of these intermediates by resonance Raman spectroscopy. Quantum chemical calculations based on a density functional theory are also performed to simulate the observed spectra. The obtained structure of the chromophore in PYP(L) has cis configuration and no hydrogen bond at the carbonyl oxygen. In PYP(M), the cis chromophore is protonated at the phenolic oxygen and forms the hydrogen bond at the carbonyl group. These results allow us to propose structural changes of the chromophore during the photocycle of PYP. The chromophore photoisomerizes from trans to cis configuration by flipping the carbonyl group to form PYP(L) with minimal perturbation of the tightly packed protein interior. Subsequent conversion to PYP(M) involves protonation on the phenolic oxygen, followed by rotation of the chromophore as a whole. This large motion of the chromophore is potentially correlated with the succeeding global conformational changes in the protein, which ultimately leads to transduction of a biological signal.     

Membrane potential stabilizes the O intermediate in liposomes containing bacteriorhodopsin.

In the bacteriorhodopsin-containing proteoliposomes, a laser flash is found to induce formation of a bathointermediate decaying in several seconds, the difference spectrum being similar to the purple-blue transition. Different pH buffers do not affect the intermediate, whereas an uncoupler, gramicidin A, and lipophilic ions accelerate decay of the intermediate or inhibit its formation. In the liposomes containing E204Q bacteriorhodopsin mutant, formation of the intermediate is suppressed. In the wild-type bacteriorhodopsin liposomes, the bathointermediate formation is pH-independent within the pH 5-7 range. The efficiency of the long-lived O intermediate formation increases at a low pH. In the wild-type as well as in the E204Q mutant purple membrane, the O intermediate decay is slowed down at slightly higher pH values than that of the purple-blue transition. It is suggested that the membrane potential affects the equilibrium between the bacteriorhodopsin ground state (Glu-204 is protonated and Asp-85 is deprotonated) and the O intermediate (Asp-85 is protonated and Glu-204 is deprotonated), stabilizing the latter by changing the relative affinity of Asp-85 and Glu-204 to H(+). At a low pH, protonation of a proton-releasing group (possibly Glu-194) in the bacteriorhodopsin ground state seems to prevent deprotonation of the Glu-204 during the photocycle. Thus, all protonatable residues of the outward proton pathway should be protonated in the O intermediate. Under such conditions, membrane potential stabilization of the O intermediate in the liposomes can be attributed to the direct effect of the potential on the pK value of Asp-85.