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.     

Coupling of hydrogen bonding to chromophore conformation and function in photoactive yellow protein

To understand in atomic detail how a chromophore and a protein interact to sense light and send a biological signal, we are characterizing photoactive yellow protein (PYP), a water-soluble, 14 kDa blue-light receptor which undergoes a photocycle upon illumination. The active site residues glutamic acid 46, arginine 52, tyrosine 42, and threonine 50 form a hydrogen bond network with the anionic p-hydroxycinnamoyl cysteine 69 chromophore in the PYP ground state, suggesting an essential role for these residues for the maintenance of the chromophore's negative charge, the photocycle kinetics, the signaling mechanism, and the protein stability. Here, we describe the role of T50 and Y42 by use of site-specific mutants. T50 and Y42 are involved in fine-tuning the chromophore's absorption maximum. The high-resolution X-ray structures show that the hydrogen-bonding interactions between the protein and the chromophore are weakened in the mutants, leading to increased electron density on the chromophore's aromatic ring and consequently to a red shift of its absorption maximum from 446 nm to 457 and 458 nm in the mutants T50V and Y42F, respectively. Both mutants have slightly perturbed photocycle kinetics and, similar to the R52A mutant, are bleached more rapidly and recover more slowly than the wild type. The effect of pH on the kinetics is similar to wild-type PYP, suggesting that T50 and Y42 are not directly involved in any protonation or deprotonation events that control the speed of the light cycle. The unfolding energies, 26.8 and 25.1 kJ/mol for T50V and Y42F, respectively, are decreased when compared to that of the wild type (29.7 kJ/mol). In the mutant Y42F, the reduced protein stability gives rise to a second PYP population with an altered chromophore conformation as shown by UV/visible and FT Raman spectroscopy. The second chromophore conformation gives rise to a shoulder at 391 nm in the UV/visible absorption spectrum and indicates that the hydrogen bond between Y42 and the chromophore is crucial for the stabilization of the native chromophore and protein conformation. The two conformations in the Y42F mutant can be interconverted by chaotropic and kosmotropic agents, respectively, according to the Hofmeister series. The FT Raman spectra and the acid titration curves suggest that the 391 nm form of the chromophore is not fully protonated. The fluorescence quantum yield of the mutant Y42F is 1.8% and is increased by an order of magnitude when compared to the wild type.     

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.     

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.     

Tryptophan fluorescence monitors structural changes accompanying signalling state formation in the photocycle of photoactive yellow protein.

Photoactive yellow protein, a small, water-soluble blue-light absorbing photoreceptor protein from Ectothiorhodospira(Halorhodospira)[space]halophila has a structure with two hydrophobic cores, of which the main one houses its light-sensitive chromophore (p-coumaric acid), separated by a central [small beta]-sheet. This photoreceptor protein contains a single tryptophan residue (W119) that is situated at the interface between the central beta-sheet and its N-terminal cap. The fluorescence properties of W119 in the dark state pG (lambda(max)= 328 nm; Phi(fl)= 0.01; nearly pH-independent) are typical for a buried tryptophan in a hydrophobic environment with significant quenching by nearby amino acid residues. Signalling state formation leads to pH-dependent fluorescence changes: At pH values <6.5 the fluorescence emission increases, with a minor blue shift of the emission maximum. Above this pH, the emission maximum of the tryptophan shifts considerably to the red, whereas its total intensity decreases. These results further support the contention that signalling state formation in PYP leads to significant changes in the structure of this protein, even at sites that are at a considerable distance from the chromophore. The nature of these changes in pB, however, depend upon the pH imposed upon the protein: At slightly alkaline pH, which presumably is closest to the pH to which this protein is exposed in vivo, these changes lead to an exposure of the part of the central beta-sheet harbouring W119. At slightly acidic pH the polarity of the environment of W119 is hardly affected by the formation of the signalling state but the quenching of its fluorescence emission, possibly by nearby amino acids, is reduced. On the other hand, its accessibility for quenching by small molecules in the solution is enhanced at acidic and alkaline pH in the signalling state (pB) compared to the dark state (pG). This latter observation points towards a more flexible structure of the N-terminal cap, having a looser interaction with the central beta-sheet in pB.     

Role of an N-terminal loop in the secondary structural change of photoactive yellow protein

Photoactive yellow protein (PYP) is photoconverted to its putative active form (PYP(M)) with global conformational change(s). The changes in the secondary structure were studied by far-UV circular dichroism (CD) and Fourier transform infrared (FTIR) spectroscopy using PYP, which lacks N-terminal 6, 15, or 23 amino acid residues (T6, T15, and T23, respectively). Irradiation of truncated PYPs induced the loss of the CD signal, where the maximal difference was located at 222 nm. The reduction of the CD signal was significantly larger than the calculated CD of the N-terminal helices, indicating that it is mainly accounted for by the unfolding and/or structural change of the helices located outside the N-terminal region. The difference FTIR spectra between dark and photosteady states recorded using the solution samples demonstrated that large absorbance changes in the amide mode of the beta-sheet were reduced and downshifted by truncation. The structural change of the beta-sheet is therefore closely correlated with the N-terminal loop. NaCl decelerates the decay of intact PYP(M) and T6(M) at low concentrations (<500 mM) but accelerates decay at high concentrations (>1000 mM). For T15(M) and T23(M), NaCl accelerates their decay at >100 mM but never decelerates their decay, suggesting that the electrostatic interaction, which plays an important role for the recovery of PYP from PYP(M), is lost by removing positions 7-15. The electrostatic interaction between this region and the beta-scaffold is likely to promote the conformational change of PYP(M) for recovery of PYP.     

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.     

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.     

Time-resolved resonance raman structural studies of the pB' intermediate in the photocycle of photoactive yellow protein

Time-resolved resonance Raman spectroscopy is used to obtain chromophore vibrational spectra of the pR, pB', and pB intermediates during the photocycle of photoactive yellow protein. In the pR spectrum, the C8-C9 stretching mode at 998 cm(-1) is approximately 60 cm(-1) lower than in the dark state, and the combination of C-O stretching and C7H=C8H bending at 1283 cm(-1) is insensitive to D2O substitution. These results indicate that pR has a deprotonated, cis chromophore structure and that the hydrogen bonding to the chromophore phenolate oxygen is preserved and strengthened in the early photoproduct. However, the intense C7H=C8H hydrogen out-of-plane (HOOP) mode at 979 cm(-1) suggests that the chromophore in pR is distorted at the vinyl and adjacent C8-C9 bonds. The formation of pB' involves chromophore protonation based on the protonation state marker at 1174 cm(-1) and on the sensitivity of the COH bending at 1148 cm(-1) as well as the combined C-OH stretching and C7H=C8H bending mode at 1252 cm(-1) to D2O substitution. The hydrogen out-of-plane Raman intensity at 985 cm(-1) significantly decreases in pB', suggesting that the pR-to-pB' transition is the stage where the stored photon energy is transferred from the distorted chromophore to the protein, producing a more relaxed pB' chromophore structure. The C=O stretching mode downshifts from 1660 to 1651 cm(-1) in the pB'-to-pB transition, indicating the reformation of a hydrogen bond to the carbonyl oxygen. Based on reported x-ray data, this suggests that the chromophore ring flips during the transition from pB' to pB. These results confirm the existence and importance of the pB' intermediate in photoactive yellow protein receptor activation.     

Initial events in the photocycle of photoactive yellow protein

The light-induced isomerization of a double bond is the key event that allows the conversion of light energy into a structural change in photoactive proteins for many light-mediated biological processes, such as vision, photosynthesis, photomorphogenesis, and photo movement. Cofactors such as retinals, linear tetrapyrroles, and 4-hydroxy-cinnamic acid have been selected by nature that provide the essential double bond to transduce the light signal into a conformational change and eventually, a physiological response. Here we report the first events after light excitation of the latter chromophore, containing a single ethylene double bond, in a low temperature crystallographic study of the photoactive yellow protein. We measured experimental phases to overcome possible model bias, corrected for minimized radiation damage, and measured absorption spectra of crystals to analyze the photoproducts formed. The data show a mechanism for the light activation of photoactive yellow protein, where the energy to drive the remainder of the conformational changes is stored in a slightly strained but fully cis-chromophore configuration. In addition, our data indicate a role for backbone rearrangements during the very early structural events.     

Light induces destabilization of photoactive yellow protein

To understand the effect of visible light on the stability of photoactive yellow protein (PYP), urea denaturation experiments were performed with PYP in the dark and with PYP(M) under continuous illumination. The urea concentrations at the midpoint of denaturation were 5.26 +/- 0.29 and 3.77 +/- 0.19 M for PYP and PYP(M), respectively, in 100 mM acetate buffer, and 5.26 +/- 0.24 and 4.11 +/- 0.12 M for PYP and PYP(M), respectively, in 100 mM citrate buffer. The free energy change upon denaturation (DeltaG(D)(H2O)), obtained from the denaturation curve, was 11.0 +/- 0.4 and 7.6 +/- 0.2 kcal/mol for PYP and PYP(M), respectively, in acetate buffer, and 11.5 +/- 0.3 and 7.8 +/- 0.1 kcal/mol for PYP and PYP(M), respectively, in citrate buffer. Even though the DeltaG(D)(H2O) value for PYP(M) is almost identical in the two buffer systems, the urea concentration at the midpoint of denaturation is lower in acetate buffer than in citrate buffer. Although their CD spectra indicate that the protein conformations of the denatured states of PYP and PYP(M) are indistinguishable, the configurations of the chromophores in their denatured structures are not necessarily identical. Both denatured states are interconvertible through PYP and PYP(M). Therefore, the free energy difference between PYP and PYP(M) is 3.4-3.7 kcal/mol for the protein moiety, plus the additional contribution from the difference in configuration of the chromophore.     

Conformational changes in the N-terminal region of photoactive yellow protein: a time-resolved diffusion study

The kinetics of conformational change in the N-terminal region of photoactive yellow protein (PYP) was studied by the time-resolved diffusion measurement. The transient grating signal that represented the protein diffusion of the ground state and pB state depended on the observation time range. An analysis of the signal based on the time-dependent diffusion coefficient clearly showed that protein diffusion changed with a time constant of 170 μs, corresponding to the pR₂ → pB′ transition. Since a previous diffusion study of N-terminal truncated PYPs had revealed that the change in the diffusion coefficient reflected the unfolding of the α-helices in the N-terminal region of PYP, the results indicate that this unfolding took place at the same rate as the pR₂ → pB′ transition. This demonstrates that the response of the conformational change in the N-terminal region was quite fast, probably due to changes in a specific hydrogen-bonding network of this domain.     

Signal transduction in the photoactive yellow protein. II. Proton transfer initiates conformational changes

Molecular dynamics simulation techniques, together with semiempirical PM3 calculations, have been used to investigate the effect of photoisomerization of the 4-hydroxy-cinnamic acid chromophore on the structural properties of the photoactive yellow protein (PYP) from Ectothiorodospira halophila. In this bacteria, exposure to blue light leads to a negative photoactic response. The calculations suggest that the isomerization does not directly destabilize the protein. However, because of the isomerization, a proton transfer from a glutamic acid residue (Glu46) to the phenolate oxygen atom of the chromophore becomes energetically favorable. The proton transfer initiates conformational changes within the protein, which are in turn believed to lead to signaling.     

Photoisomerization and photoionization of the photoactive yellow protein chromophore in solution

Dispersed pump-dump-probe spectroscopy has the ability to characterize and identify the underlying ultrafast dynamical processes in complicated chemical and biological systems. This technique builds on traditional pump-probe techniques by exploring both ground- and excited-state dynamics and characterizing the connectivity between constituent transient states. We have used the dispersed pump-dump-probe technique to investigate the ground-state dynamics and competing excited-state processes in the excitation-induced ultrafast dynamics of thiomethyl p-coumaric acid, a model chromophore for the photoreceptor photoactive yellow protein. Our results demonstrate the parallel formation of two relaxation pathways (with multiple transient states) that jointly lead to two different types of photochemistry: cis-trans isomerization and detachment of a hydrated electron. The relative transition rates and quantum yields of both pathways have been determined. We find that the relaxation of the photoexcited chromophores involves multiple, transient ground-state intermediates and the chromophore in solution does not generate persistent photoisomerized products, but instead undergoes photoionization resulting in the generation of detached electrons and radicals. These results are of great value in interpreting the more complex dynamical changes in the optical properties of the photoactive yellow protein.     

Absorption spectra of photoactive yellow protein chromophores in vacuum

The absorption spectra of two photoactive yellow protein model chromophores have been measured in vacuum using an electrostatic ion storage ring. The absorption spectrum of the isolated chromophore is an important reference for deducing the influence of the protein environment on the electronic energy levels of the chromophore and separating the intrinsic properties of the chromophore from properties induced by the protein environment. In vacuum the deprotonated trans-thiophenyl-p-coumarate model chromophore has an absorption maximum at 460 nm, whereas the photoactive yellow protein absorbs maximally at 446 nm. The protein environment thus only slightly blue-shifts the absorption. In contrast, the absorption of the model chromophore in aqueous solution is significantly blue-shifted (lambda(max) = 395 nm). A deprotonated trans-p-coumaric acid has also been studied to elucidate the effect of thioester formation and phenol deprotonation. The sum of these two changes on the chromophore induces a red shift both in vacuum and in aqueous solution.     

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.     

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.     

Measurement and global analysis of the absorbance changes in the photocycle of the photoactive yellow protein from Ectothiorhodospira halophila.

The photocycle of the photoactive yellow protein (PYP) from Ectothiorhodospira halophila was examined by time-resolved difference absorption spectroscopy in the wavelength range of 300-600 nm. Both time-gated spectra and single wavelength traces were measured. Global analysis of the data established that in the time domain between 5 ns and 2 s only two intermediates are involved in the room temperature photocycle of PYP, as has been proposed before (Meyer T.E., E. Yakali, M. A. Cusanovich, and G. Tollin. 1987. Biochemistry. 26:418-423; Meyer, T. E., G. Tollin, T. P. Causgrove, P. Cheng, and R. E. Blankenship. 1991. Biophys. J. 59:988-991). The first, red-shifted intermediate decays biexponentially (60% with tau = 0.25 ms and 40% with tau = 1.2 ms) to a blue-shifted intermediate. The last step of the photocycle is the biexponential (93% with tau = 0.15 s and 7% with tau = 2.0 s) recovery to the ground state of the protein. Reconstruction of the absolute spectra of these photointermediates yielded absorbance maxima of about 465 and 355 nm for the red- and blue-shifted intermediate with an epsilon max at about 50% and 40% relative to the epsilon max of the ground state. The quantitative analysis of the photocycle in PYP described here paves the way to a detailed biophysical analysis of the processes occurring in this photoreceptor molecule.     

Light-induced global conformational change of photoactive yellow protein in solution

The light-induced global conformational change of photoactive yellow protein was directly observed by small-angle X-ray scattering (SAXS). The N-terminal 6, 15, or 23 amino acid residues were enzymatically truncated (T6, T15, or T23, respectively), and their near-UV intermediates were accumulated under continuous illumination for SAXS measurements. The Kratky plot demonstrated that illumination induced partial loss of globularity. The change in globularity was marked in T6 but very small in T15 and T23, suggesting that structural change in positions 7-15 mainly reduces the globularity. The radius of gyration (R(g)) estimated by Guinier plot was increased by 1.1 A for T6 and 0.7 A for T15 and T23 upon illumination. As T23 lacks most of the N-terminal loop, structural change in the main part composed of the PAS core, helical connector, and beta-scaffold caused an increase of R(g) by 0.7 A. The structural change of positions 7-15 caused an additional increase by 0.4 A. The decrease of R(g) upon truncation of positions 7-15 for dark state was 0.3 A, while that for the intermediate was 0.7 A, suggesting that this region moves outward on formation of the intermediate. These results indicate that a light-induced structural change of PYP takes place in the main part and N-terminal 15 amino acid residues. The former induces only dimensional increase, but the latter results in additional change in shape.     

Mimic of photocycle by a protein folding reaction in photoactive yellow protein

The blue light receptor photoactive yellow protein (PYP) displays rhodopsin-like photochemistry based on the trans to cis photoisomerization of its p-coumaric acid chromophore. Here, we report that protein refolding from the acid-denatured state of PYP mimics the last photocycle transition in PYP. This implies a direct link between transient protein unfolding and photosensory signal transduction. We utilize this link to study general issues in protein folding. Chromophore trans to cis photoisomerization in the acid-denatured state strongly decelerates refolding, and converts the pH dependence of the barrier for refolding from linear to nonlinear. We propose transition state movement to explain this phenomenon. The cis chromophore significantly stabilizes the acid-denatured state, but acidification of PYP results in the accumulation of the acid-denatured state containing a trans chromophore. This provides a clear example of kinetic control in a protein unfolding reaction. These results demonstrate the power of PYP as a light-triggered model system to study protein folding.