Spectroscopic characterization of the photocycle intermediates of photoactive yellow protein.

The absorption spectra of photocycle intermediates of photoactive yellow protein mutants were compared with those of the corresponding intermediates of wild type to probe which amino acid residues interact with the chromophore in the intermediate states. B and H intermediates were produced by irradiation and trapped at 80 K, and L intermediates at 193 K. The absorption spectra of these intermediates produced from R52Q were identical to those from wild type, whereas those from E46Q and T50V were 7-15 nm red-shifted as those in the dark states. The absorption spectra of M intermediates were measured by flash photolysis at room temperature. Those of Y42F, T50V, and R52Q were identical to that of wild type, whereas that of E46Q was 11 nm red-shifted. Assuming that the intermediates of mutants have a structure comparable to that of wild type, these findings suggest the following: Glu46 interacts with the chromophore throughout the photocycle, interaction between the chromophore and Thr50 as well as Tyr42 is lost upon the formation of M intermediate, and Arg52 never interacts with the chromophore directly. The hydrogen-bonding network around the phenolic oxygen of the chromophore would be thus maintained until L intermediate decays, and the global conformational change would take place by the loss of the hydrogen bond between the chromophore and Tyr42. This model conflicts with some of the results of previous crystallographic studies, suggesting that the reaction mechanism in the crystal may be different from that in solution.     

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

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

A role of methionine 100 in facilitating PYP(M)-decay process in the photocycle of photoactive yellow protein

PYP (photoactive yellow protein) is a photoreceptor protein, which is activated upon photo-isomerization of the p-coumaric acid chromophore and is inactivated as the chromophore is thermally back-isomerized within a second (in PYP(M)-to-PYP(dark) conversion). Here we have examined the mechanism of the rapid thermal isomerization by analyzing mutant PYPs of Met100, which was previously shown to play a major role in facilitating the reaction [Devanathan, S. et al. (1998) Biochemistry 37, 11563-11568]. The mutation to Lys, Leu, Ala, or Glu decelerated the dark state recovery by one to three orders of magnitude. By evaluating temperature-dependence of the kinetics, it was found that the retardation resulted unequivocally from elevations of activation enthalpy (DeltaH( double dagger )) but not the other parameters such as activation entropy or heat capacity changes. Another effect exerted by the mutations was an up-shift of the apparent pK(a) of the chromophore [the pK(a) of a titratable group (X) that controls the pK(a) of the chromophore] in the PYP(M)-decay process. The pK(a) up-shift and the DeltaH( double dagger ) elevation show an approximately linear correlation. We, therefore, postulate that the role of Met100 is to reduce the energy barrier of the PYP(M)-decay process by an indirect interaction through X and that the process is thereby facilitated.     

Purification, characterization and crystallization of the core complex from thermophilic purple sulfur bacterium Thermochromatium tepidum

A light-harvesting-reaction center (LH1-RC) core complex has been highly purified from a thermophilic purple sulfur bacterium, Thermochromatium tepidum. The bacteriochlorophyll (BChl) a molecules in the LH1 exhibit a Q(y) transition at 914 nm, more than 25 nm red-shift from those of its mesophilic counterparts. The LH1-RC complex was isolated in a monomeric form as confirmed by sucrose density gradient centrifugation, blue native PAGE and size-exclusion chromatography. Four subunits (L, M, H and a tetraheme cytochrome) in RC and two polypeptides (alpha and beta) in LH1 were identified. Spirilloxanthin was determined to be the predominant carotenoid in the core complex. The purified core complex was highly stable, no significant change in the LH1 Q(y) transition was observed over 10 days of incubation at room temperature in dark. Circular dichroism spectrum of the LH1 complex was characterized by low intensity and nonconservative spectral shape, implying a high symmetry of the large LH1 ring and interaction between the BChl a and carotenoid molecules. A dimeric feature of the BChl a molecules in LH1 was revealed by magnetic circular dichroism spectrum. Crystals of the core complex were obtained which diffracted X-rays to about 10 A.     

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.     

Gene sequencing and characterization of the light-harvesting complex 2 from thermophilic purple sulfur bacterium Thermochromatium tepidum

In this study, gene sequences coding for the light-harvesting (LH) 2 polypeptides from a thermophilic purple sulfur bacterium Thermochromatium tepidum are reported and characterization of the LH2 complex is described. Three sets of pucBA genes have been identified, and the gene products have been analyzed by electrophoresis and reversed-phase chromatography. The result shows that all of the genes are expressed but the distribution of the expression is not uniform. The gene products undergo post-translational modification, where two of the β-polypeptides appear to be N-terminally methylated. Absorption spectrum of the purified LH2 complex exhibits Q _y transitions at 800 and 854?nm in dodecyl β-maltopyranoside solution, and the circular dichroism spectrum shows a “molischianum”-like characteristic. No spectral change was observed for the LH2 when the bacterium was cultured under different conditions of light intensity. In lauryl dimethylamine N-oxide (LDAO) solution, significant changes in the absorption spectrum were observed. The B850 peak decreased and blue-shifted with increasing the LDAO concentration, whereas the B800 intensity increased without change in the peak position. The spectral changes can be partially or almost completely reversed by addition of metal ions, and the divalent cations seem to be more effective. The results indicate that ionic interactions may exist between LH2, detergent molecules and metal ions. Possible mechanisms involved in the detergent- and cation-induced spectral changes are discussed.     

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.     

Crystallographic characterization of a photoactive yellow protein with photochemistry similar to sensory rhodopsin

A photoactive yellow protein purified from the phototrophic bacterium Ectothiorhodospira halophila, has been crystallized by vapor diffusion from ammonium sulfate solution. The hexagonal crystals are in space group P6(3) with unit cell dimensions a = b = 66.89, c = 40.68 A and appear to have one 15,000-dalton protein in the asymmetric unit. Photoactive yellow protein contains a chromophore with retinal-like properties; its color can be reversibly bleached, by visible light, with kinetics similar to those of sensory rhodopsin. The crystals can also be bleached by an intense visible light source without cracking, but are not bleached by x-rays. This suggests that structures can be obtained for both bleached and colored conformations of the protein-bound chromophore. The crystals diffract strongly to at least 1.3 A resolution, are resistant to radiation damage, and are suitable for a high resolution structure determination. The covalently bound chromophore and photobleaching characteristics of the protein offer unique opportunities to study protein conformational change and refolding as well as to understand the mechanisms of light-induced conformational change at atomic resolution.     

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.     

PAS domain receptor photoactive yellow protein is converted to a molten globule state upon activation

Biological signaling generally involves the activation of a receptor protein by an external stimulus followed by protein-protein interactions between the activated receptor and its downstream signal transducer. The current paradigm for the relay of signals along a signal transduction chain is that it occurs by highly specific interactions between fully folded proteins. However, recent results indicate that many regulatory proteins are intrinsically unstructured, providing a serious challenge to this paradigm and to the nature of structure-function relationships in signaling. Here we study the structural changes that occur upon activation of the blue light receptor photoactive yellow protein (PYP). Activation greatly reduces the tertiary structure of PYP but leaves the level secondary structure largely unperturbed. In addition, activated PYP exposes previously buried hydrophobic patches and allows significant solvent penetration into the core of the protein. These traits are the distinguishing hallmarks of molten globule states, which have been intensively studied for their role in protein folding. Our results show that receptor activation by light converts PYP to a molten globule and indicate stimulus-induced unfolding to a partially unstructured molten globule as a novel theme in signaling.     

Rhodobacter capsulatus photoactive yellow protein: genetic context, spectral and kinetics characterization, and mutagenesis

A gene for photoactive yellow protein (PYP) was previously cloned from Rhodobacter capsulatus (Rc), and we have now found it to be associated with genes for gas vesicle formation in the recently completed genome sequence. However, the PYP had not been characterized as a protein. We have now produced the recombinant RcPYP in Escherichia coli as a glutathione-S-transferase (GST) fusion protein, along with the biosynthetic enzymes, resulting in the formation of holo-RcPYP following cleavage of the GST tag. The absorption spectrum (with characteristic peaks at 435 and 375 nm) and the photocycle kinetics, initiated by a laser flash at 445 nm, are generally similar to those of Rhodobacter sphaeroides (RsPYP) but are significantly different from those of the prototypic PYP from Halorhodospira halophila (HhPYP), which has a single peak at 446 nm and has slower recovery. RcPYP also is photoactive when excited with near-ultraviolet laser light, but the end point is then above the preflash baseline. This suggests that some of the PYP chromophore is present in the cis-protonated conformation in the resting state. The excess 435 nm form in RcPYP, built up from repetitive 365 nm laser flashes, returns to the preflash baseline with an estimated half-life of 2 h, which is markedly slower than that for the same reaction in RsPYP. Met100 has been reported to facilitate cis-trans isomerization in HhPYP, yet both Rc and RsPYPs have Lys and Gly substitutions at positions 99 and 100 (using HhPYP numbering throughout) and have 100-fold faster recovery kinetics than does HhPYP. However, the G100M and K99Q mutations of RcPYP have virtually no effect on kinetics. Apparently, the RcPYP M100 is in a different conformation, as was recently found for the PYP domain of Rhodocista centenaria Ppr. The cumulative results show that the two Rhodobacter PYPs are clearly distinct from the other species of PYP that have been characterized. These properties also suggest a different functional role, that we postulate to be in regulation of gas vesicle genes, which are known to be light-regulated in other species.     

Contrasting the excited-state dynamics of the photoactive yellow protein chromophore: protein versus solvent environments

Wavelength- and time-resolved fluorescence experiments have been performed on the photoactive yellow protein, the E46Q mutant, the hybrids of these proteins containing a nonisomerizing “locked” chromophore, and the native and locked chromophores in aqueous solution. The ultrafast dynamics of these six systems is compared and spectral signatures of isomerization and solvation are discussed. We find that the ultrafast red-shifting of fluorescence is associated mostly with solvation dynamics, whereas isomerization manifests itself as quenching of fluorescence. The observed multiexponential quenching of the protein samples differs from the single-exponential lifetimes of the chromophores in solution. The locked chromophore in the protein environment decays faster than in solution. This is due to additional channels of excited-state energy dissipation via the covalent and hydrogen bonds with the protein environment. The observed large dispersion of quenching timescales observed in the protein samples that contain the native pigment favors both an inhomogeneous model and an excited-state barrier for isomerization.     

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.     

Low-temperature Fourier transform infrared spectroscopy of photoactive yellow protein

The photocycle intermediates of photoactive yellow protein (PYP) were characterized by low-temperature Fourier transform infrared spectroscopy. The difference FTIR spectra of PYP(B), PYP(H), PYP(L), and PYP(M) minus PYP were measured under the irradiation condition determined by UV-visible spectroscopy. Although the chromophore bands of PYP(B) were weak, intense sharp bands complementary to the 1163-cm(-1) band of PYP, which show the chromophore is deprotonated, were observed at 1168-1169 cm(-1) for PYP(H) and PYP(L), indicating that the proton at Glu46 is not transferred before formation of PYP(M). Free trans-p-coumaric acid had a 1294-cm(-1) band, which was shifted to 1288 cm(-1) in the cis form. All the difference FTIR spectra obtained had the pair of bands corresponding to them, indicating that all the intermediates have the chromophore in the cis configuration. The characteristic vibrational modes at 1020-960 cm(-1) distinguished the intermediates. Because these modes were shifted by deuterium-labeling at the ethylene bond of the chromophore while labeling at the phenol part had no effect, they were attributed to the ethylene bond region. Hence, structural differences among the intermediates are present in this region. Bands at about 1730 cm(-1), which show that Glu46 is protonated, were observed for all intermediates except for PYP(M). Because the frequency of this mode was constant in PYP(B), PYP(H), and PYP(L), the environment of Glu46 is conserved in these intermediates. The photocycle of PYP would therefore proceed by changing the structure of the twisted ethylene bond of the chromophore.     

Effect of organic anions on the photoreaction of photoactive yellow protein

In order to clarify changes in the structure and surface properties of photoactive yellow protein (PYP) upon light absorption, the spectroscopic properties and solution structure of its photo-intermediate (PYP(M)) were examined in the presence of various anions. At identical ionic strengths, citrate slowed the decay rate of PYP(M) more than acetate. Although the absorption spectrum in the dark was not affected by organic anions, citrate induced a 5-nm blue shift of the absorption maximum for PYP(M). Solution X-ray scattering experiments indicated that the radius of gyration (Rg) and apparent molecular weight in the dark were constant in all buffer systems. However, the Rg of PYP(M) in citrate buffer at high concentration was 16.2 (+/-0.2) A, while the Rg of PYP(M) in acetate buffer was 15.6 (+/-0.2) A. The apparent molecular weight increased 7% upon PYP(M) formation in citrate buffer at high concentration compared to other conditions. These results suggest that citrate molecules specifically bind to PYP(M). A cluster of basic amino acid residues with a hydrogen bond donor would be exposed upon PYP(M) formation and responsible for the specific binding of citrate.     

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.     

Light-induced unfolding of photoactive yellow protein mutant M100L

Light-activation of the PAS domain protein photoactive yellow protein (PYP) is believed to trigger a negative phototactic response in the phototropic bacterium Halorhodospira halophila. To investigate transient conformational changes of the PYP photocycle, we utilized the PYP mutant M100L that displays an increased lifetime of the putative signaling-state photointermediate PYP(M) by 3 orders of magnitude, as previously reported for the M100A mutant [Devanathan, S., Genick, U. K., Canestrelli, I. L., Meyer, T. E., Cusanovich, M. A., Getzoff, E. D., and Tollin, G. Biochemistry (1998) 37, 11563-11568]. The FTIR difference spectrum of PYP(M) and the ground state of M100L demonstrated extensive peptide-backbone structural changes as observed in the FTIR difference spectrum of the wild-type protein and PYP(M). The conformational change investigated by CD spectroscopy in the far-UV region showed reduction of the alpha-helical content by approximately 40%, indicating a considerable amount of changes in the secondary structure. The optical activity of the p-coumaric acid chromophore completely vanished upon PYP(M) in contrast to the dark state, indicating deformation of the binding pocket structure in PYP(M). The tertiary structural changes were further monitored by small-angle X-ray scattering measurements, which demonstrated a significant increase of the radius of gyration of the molecule by approximately 5% in PYP(M). These structural changes were reversed concomitantly with the chromophore anionization upon the dark state recovery. The observed changes of the quantities provided a more vivid view of the structural changes of the mutant PYP in going from PYP(M) to PYP(dark), which can be regarded as a process of folding of the secondary and the tertiary structures of the "PAS" domain structure, coupled with the p-coumaric acid chromophore deprotonation and isomerization.     

The two photocycles of photoactive yellow protein from Rhodobacter sphaeroides

The absorption spectrum of the photoactive yellow protein from Rhodobacter sphaeroides (R-PYP) shows two maxima, absorbing at 360 nm (R-PYP(360)) and 446 nm (R-PYP(446)), respectively. Both forms are photoactive and part of a temperature- and pH-dependent equilibrium (Haker, A., Hendriks, J., Gensch, T., Hellingwerf, K. J., and Crielaard, W. (2000) FEBS Lett. 486, 52-56). At 20 degrees C, for PYP characteristic, the 446-nm absorbance band displays a photocycle, in which the depletion of the 446-nm ground state absorption occurs in at least three phases, with time constants of <30 ns, 0.5 micros, and 17 micros. Intermediates with both blue- and red-shifted absorption maxima are transiently formed, before a blue-shifted intermediate (pB(360), lambda(max) = 360 nm) is established. The photocycle is completed with a monophasic recovery of the ground state with a time constant of 2.5 ms. At 7 degrees C these photocycle transitions are slowed down 2- to 3-fold. Upon excitation of R-PYP(360) with a UV-flash (330 +/- 50 nm) a species with a difference absorption maximum at approximately 435 nm is observed that returns to R-PYP(360) on a minute time scale. Recovery can be accelerated by a blue light flash (450 nm). R-PYP(360) and R-PYP(446) differ in their overall protein conformation, as well as in the isomerization and protonation state of the chromophore, as determined with the fluorescent polarity probe Nile Red and Fourier Transform Infrared spectroscopy, respectively.     

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.