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     

On the Configurational and Conformational Changes in Photoactive Yellow Protein that Leads to Signal Generation in Ectothiorhodospira halophila

Photoactive Yellow Protein (PYP), a phototaxis photoreceptor from Ectothiorhodospira halophila, is a small water-soluble protein that iscrystallisable and excellently photo-stable. It can be activated with light(^max= 446 nm), to enter a series of transientintermediates that jointly form the photocycle of this photosensor protein.The most stable of these transient states is the signalling state forphototaxis, pB.The spatial structure of the ground state of PYP, pG and the spectralproperties of the photocycle intermediates have been very well resolved.Owing to its excellent chemical- and photochemical stability, also the spatialstructure of its photocycle intermediates has been characterised with X-raydiffraction and multinuclear NMR spectroscopy. Surprisingly, the resultsobtained showed that their structure is dependent on the molecular contextin which they are formed. Therefore, a large range of diffraction-,scattering- and spectroscopic techniques is now being employed to resolvein detail the dynamical changes of the structure of PYP while it progressesthrough its photocycle. This approach has led to considerable progress,although some techniques still result in mutually inconsistent conclusionsregarding aspects of the structure of particular intermediates.Recently, significant progress has also been made with simulations withmolecular dynamics analyses of the initial events that occur in PYP uponphoto activation. The great challenge in this field is to eventually obtainagreement between predicted dynamical alterations in PYP structure, asobtained with the MD approach and the actually measured dynamicalchanges in its structure as evolving during photocycle progression.     

Themodynamic and transport properties of intermediate states of the photocyclic reaction of photoactive yellow protein

Themodynamic and transport properties of intermediate states of the photocyclic reaction of photoactive yellow protein (PYP) were studied by a combination of the pulsed laser-induced transient grating (TG), transient lens (TrL), and photoacoustic (PA) spectroscopies from tens of nanoseconds to hundreds of milliseconds. The diffusion coefficients (D) of PYP in the ground state (pG) and of the second intermediate state (pB) were determined by the TG analysis, and it was found that D of pG is about 1.2 times larger than D of pB. At the same time, D at various denatured conditions were measured using guanidine hydrochloride as the denaturant. D of completely unfolded protein is about 0.4 times that of the native form. The enthalpy of pB is estimated to be 60 kJ/mol by the TrL method with an assumption that the volume change of pB is not sensitive to the temperature. Since the enthalpy of the first intermediate state (pR) is as high as 160 kJ/mol, it implies that most of the photon energy is stored as the strain of the protein in pR, and this may be the driving force for the successive reaction to pB. From the temperature dependence of the volume change, the difference in the thermal expansion coefficients between pG and pR was calculated. All of the characteristic features of PYP, the negative volume change, the larger thermal expansion coefficient, and the slower diffusion process, indicate that the intermediate pR and pB are reasonably interpreted in terms of the unfolded (loosened) protein structure.     

Controlled reduction of the humidity induces a shortcut recovery reaction in the photocycle of photoactive yellow protein

The photocycle of the blue-light photoreceptor protein Photoactive Yellow Protein (PYP) was studied at reduced relative humidity (RH). Photocycle kinetics and spectra were measured in thin films of PYP in which the relative humidity was set at values between 29 and 98% RH with saturated solutions of various salts. We show that in this range, approximately 200 water molecules per PYP molecule are released from the film. As humidity decreased, photocycle transition rates changed, until at low humidity (RH < 50%) an authentic photocycle was no longer observed and the absorption spectrum of the dark, equilibrium state of PYP started to shift to 355 nm, that is, to a form resembling that of pB(dark). At moderately reduced humidity (i.e., >50% RH), an authentic photocycle is still observed, although its characteristics differ from those in solution. As humidity decreases, the rate of ground state recovery increases, while the rate of depletion of the first red-shifted intermediate pR dramatically decreases. The latter observation contrasts all so-far known modulations of the rate of the transition of the red-shifted- to the blue-shifted intermediates of PYP, which is consistently accelerated by all other modulations of the mesoscopic context of the protein. Under these same conditions, the long-lived, blue-shifted intermediate was formed not only with slower kinetics than in solution but also to a smaller extent. Global analysis of these data indicates that in this low humidity environment the photocycle can take a different route than in solution, that is, part of pG recovers directly from pR. These experiments on wild-type PYP, in combination with observations on a variant of PYP obtained by site-directed mutagenesis (the E46Q mutant protein), further document the context dependence of the photocycle transitions of PYP and are relevant for the interpretation of results obtained in both spectroscopic and diffraction studies with crystalline PYP.     

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.     

Photoinduced volume change and energy storage associated with the early transformations of the photoactive yellow protein from Ectothiorhodospira halophila.

The photocycle of the photoactive yellow protein (PYP) isolated from Ectothiorhodospira halophila was analyzed by flash photolysis with absorption detection at low excitation photon densities and by temperature-dependent laser-induced optoacoustic spectroscopy (LIOAS). The quantum yield for the bleaching recovery of PYP, assumed to be identical to that for the phototransformation of PYP (pG), to the red-shifted intermediate, pR, was phi R = 0.35 +/- 0.05, much lower than the value of 0.64 reported in the literature. With this value and the LIOAS data, an energy content for pR of 120 kJ/mol was obtained, approximately 50% lower than for excited pG. Concomitant with the photochemical process, a volume contraction of 14 ml/photoconverted mol was observed, comparable with the contraction (11 ml/mol) determined for the bacteriorhodopsin monomer. The contraction in both cases is interpreted to arise from a protein reorganization around a phototransformed chromophore with a dipole moment different from that of the initial state. The deviations from linearity of the LIOAS data at photon densities > 0.3 photons per molecule are explained by absorption by pG and pR during the laser pulse duration (i.e., a four-level system, pG, pR, and their respective excited states). The data can be fitted either by a simple saturation process or by a photochromic equilibrium between pG and pR, similar to that established between the parent chromoprotein and the first intermediate(s) in other biological photoreceptors. This nonlinearity has important consequences for the interpretation of the data obtained from in vitro studies with powerful lasers.     

The solution structure of a transient photoreceptor intermediate: Delta25 photoactive yellow protein

The N-terminally truncated variant of photoactive yellow protein (Delta25-PYP) undergoes a very similar photocycle as the corresponding wild-type protein (WT-PYP), although the lifetime of its light-illuminated (pB) state is much longer. This has allowed determination of the structure of both its dark- (pG) as well as its pB-state in solution by nuclear magnetic resonance (NMR) spectroscopy. The pG structure shows a well-defined fold, similar to WT-PYP and the X-ray structure of the pG state of Delta25-PYP. In the long-lived photocycle intermediate pB, the central beta sheet is still intact, as well as a small part of one alpha helix. The remainder of pB is unfolded and highly flexible, as evidenced by results from proton-deuterium exchange and NMR relaxation studies. Thus, the partially unfolded nature of the presumed signaling state of PYP in solution, as suggested previously, has now been structurally demonstrated.     

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.     

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.     

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.     

Structural change of site-directed mutants of PYP: new dynamics during pR state

The energetics, protein dynamics, and diffusion coefficients of three mutants of photoactive yellow protein, R52Q, P68A, and W119G, were studied by the transient grating and pulsed laser-induced photoacoustic method. We observed a new dynamics with a lifetime of approximately 1 micro s in the transient grating signal, which is silent by the light absorption technique. This fact indicates that, after the structure change around the chromophore is completed (pR(1)), the protein part located far from the chromophore is still moving to finally create another pR (pR(2)) species, which can transform to the next intermediate, pB. Although the kinetics of pR(2)-->pB-->pG are very different depending on the mutants, the enthalpies of the first long-lived (in micro seconds, 100-micro s range) intermediate species (pR(2)) are similar and very high for all mutants. The diffusion coefficients of the parent (pG) and pB species of the mutants are also similar to that of the wild-type photoactive yellow protein. From the temperature dependence of the volume change, the difference in the thermal expansion coefficients taken as indicator of the flexibility of the structure between pG and pR(2) is measured. They are also similar to that of the wild-type photoactive yellow protein. These results suggest that the protein structures of pR(2) and pB in these mutants are globally different from that of pG, and this structural change is not altered so much by the single amino acid residue mutation. This is consistent with the partially unfolded nature of these intermediate species. On the other hand, the volume changes during pR(1)-->pR(2) are sensitive to the mutations, which may suggest that the volume change reflects a rather local character of the structure, such as the chromophore-protein interaction.     

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

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

Conformational changes of PYP monitored by diffusion coefficient: effect of N-terminal alpha-helices

Conformational changes in the light illuminated intermediate (pB) of photoactive yellow protein (PYP) were studied from a viewpoint of the diffusion coefficient (D) change of several N-truncated PYPs, which lacked the N-terminal 6, 15, or 23 amino acid residues (T6, T15, and T23, respectively). For intact PYP (i-PYP), D of pB (D(pB)) was approximately 11% lower than that (D(pG)) of the ground state (pG) species. The difference in D (D(pG) - D(pB)) decreased upon cleavage of the N-terminal region in the order of i-PYP>T6>T15>T23. This trend clearly showed that conformational change in the N-terminal group is the main reason for the slower diffusion of pB. This slower diffusion was interpreted in terms of the unfolding of the two alpha-helices in the N-terminal region, increasing the intermolecular interactions due to hydrogen bonding with water molecules. The increase in friction per one residue by the unfolding of the alpha-helix was estimated to be 0.3 x 10(-12) kg/s. The conformational change in the N-terminal group upon photoillumination is 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.     

Synthesis,properties, and biological activity of boranophosphate analogs of the mRNA cap: versatile tools for manipulation of therapeutically relevant cap-dependent processes

Modified mRNA cap analogs aid in the study of mRNA-related processes and may enable creation of novel therapeutic interventions. We report the synthesis and properties of 11 dinucleotide cap analogs bearing a single boranophosphate modification at either the α-, β- or γ-position of the 5′,5′-triphosphate chain. The compounds can potentially serve either as inhibitors of translation in cancer cells or reagents for increasing expression of therapeutic proteins in vivo from exogenous mRNAs. The BH₃-analogs were tested as substrates and binding partners for two major cytoplasmic cap-binding proteins, DcpS, a decapping pyrophosphatase, and eIF4E, a translation initiation factor. The susceptibility to DcpS was different between BH₃-analogs and the corresponding analogs containing S instead of BH₃ (S-analogs). Depending on its placement, the boranophosphate group weakened the interaction with DcpS but stabilized the interaction with eIF4E. The first of the properties makes the BH₃-analogs more stable and the second, more potent as inhibitors of protein biosynthesis. Protein expression in dendritic cells was 2.2- and 1.7-fold higher for mRNAs capped with m₂^7,2′-OGpp_BH3pG D1 and m₂^7,2′-OGpp_BH3pG D2, respectively, than for in vitro transcribed mRNA capped with m₂^7,3′-OGpppG. Higher expression of cancer antigens would make mRNAs containing m₂^7,2′-OGpp_BH3pG D1 and m₂^7,2′-OGpp_BH3pG D2 favorable for anticancer immunization.     

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.     

Chemical probing of RNA with the hydroxyl radical at single-atom resolution

While hydroxyl radical cleavage is widely used to map RNA tertiary structure, lack of mechanistic understanding of strand break formation limits the degree of structural insight that can be obtained from this experiment. Here, we determine how individual ribose hydrogens of sarcin/ricin loop RNA participate in strand cleavage. We find that substituting deuterium for hydrogen at a ribose 5′-carbon produces a kinetic isotope effect on cleavage; the major cleavage product is an RNA strand terminated by a 5′-aldehyde. We conclude that hydroxyl radical abstracts a 5′-hydrogen atom, leading to RNA strand cleavage. We used this approach to obtain structural information for a GUA base triple, a common tertiary structural feature of RNA. Cleavage at U exhibits a large 5′ deuterium kinetic isotope effect, a potential signature of a base triple. Others had noted a ribose-phosphate hydrogen bond involving the G 2′-OH and the U phosphate of the GUA triple, and suggested that this hydrogen bond contributes to backbone rigidity. Substituting deoxyguanosine for G, to eliminate this hydrogen bond, results in a substantial decrease in cleavage at G and U of the triple. We conclude that this hydrogen bond is a linchpin of backbone structure around the triple.     

Proline 54 trans-cis isomerization is responsible for the kinetic partitioning at the last-step photocycle of photoactive yellow protein

Photoactive yellow protein (PYP), a blue-light photoreceptor for Ectothiorhodospira halophila, has provided a unique system for studying protein folding that is coupled with a photocycle. Upon receptor activation by blue light, PYP proceeds through a photocycle that includes a partially folded signaling state. The last-step photocycle is a thermal recovery reaction from the signaling state to the native state. Bi-exponential kinetics had been observed for the last-step photocycle; however, the slow phase of the bi-exponential kinetics has not been extensively studied. Here we analyzed both fast and slow phases of the last-step photocycle in PYP. From the analysis of the denaturant dependence of the fast and slow phases, we found that the last-step photocycle proceeds through parallel channels of the folding pathway. The burial of the solvent-accessible area was responsible for the transition state of the fast phase, while structural rearrangement from the compact state to the native state was responsible for the transition state of the slow phase. The photocycle of PYP was linked to the thermodynamic cycle that includes both unfolding and refolding of the fast- and slow-phase intermediates. In order to test the hypothesis of proline-limited folding for the slow phase, we constructed two proline mutants: P54A and P68A. We found that only a single phase of the last-step photocycle was observed in P54A. This suggests that there is a low energy barrier between trans to cis conformation in P54 in the light-induced state of PYP, and the resulting cis conformation of P54 generates a slow-phase kinetic trap during the photocycle-coupled folding pathway of PYP.     

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 I₂′. The pH dependence of the equilibrium between the transient photocycle intermediates I₂ and I₂′ was investigated. The formation of I₂′ from I₂ 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: I₁, I₂, and I₂′. Their spectra were determined using the extrapolated difference method. I₂ and I₂′ 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 I₁, I₂, and I₂′ intermediates were determined from the wavelength-dependent transient absorbance changes at each pH, assuming that their spectra are pH-independent. After the formation of I₂′ (~2 ms), these three intermediates are in equilibrium and decay together to the initial dark state. The equilibrium between I₂ and I₂′ is pH dependent with a pK_a of 6.4 and with I₂′ 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. I₂ and I₂′ are photoreversed with reversal times of ~55 μs and several hundred microseconds, respectively. The corresponding signal amplitudes are pH dependent with a pK_a of ~6.1. Photoreversal from I₂′ dominates above the pK_a. The transient accumulation of I₂′, the active state of photoactive yellow protein, is thus controlled by the proton concentration. The rate constant k₃ for the recovery to the initial dark state also has a pK_a of ~6.3. This equality of the equilibrium and kinetic pK_a values is not accidental and suggests that k₃ is proportional to [I₂′].