Photoactive Yellow Protein, A New Type of Photoreceptor Protein: Will This “Yellow Lab” Bring Us Where We Want to Go?

Ultrafast Dynamics of Isolated Model Photoactive Yellow Protein Chromophores: “Chemical Perturbation Theory” in the Laboratory

Pump-probe and pump-dump probe experiments have been performed on several isolated model chromophores of the photoactive yellow protein (PYP). The observed transient absorption spectra are discussed in terms of the spectral signatures ascribed to solvation, excited-state twisting, and vibrational relaxation. It is observed that the protonation state has a profound effect on the excited-state lifetime of p-coumaric acid. Pigments with ester groups on the coumaryl tail end and charged phenolic moieties show dynamics that are significantly different from those of other pigments. Here, an unrelaxed ground-state intermediate could be observed in pump-probe signals. A similar intermediate could be identified in the sinapinic acid and in isomerization-locked chromophores by means of pump-dump probe spectroscopy; however, in these compounds it is less pronounced and could be due to ground-state solvation and/or vibrational relaxation. Because of strong protonation-state dependencies and the effect of electron donor groups, it is argued that charge redistribution upon excitation determines the twisting reaction pathway, possibly through interaction with the environment. It is suggested that the same pathway may be responsible for the initiation of the photocycle in native PYP.

Carboxylate anions binding and sensing by a novel tetraazamacrocycle containing ferrocene as receptor

A tetraazamacrocycle containing ferrocene moieties has been synthesized and characterized. The tetraprotonated form of this compound was evaluated as a receptor (R) for anion recognition of several substrates (S), Cl(-), PF(6)(-), HSO(4)(-), H(2)PO(4)(-) and carboxylates, such as p-nitrobenzoate (p-nbz(-)), phthalate (ph(2-)), isophthalate (iph(2-)) and dipicolinate (dipic(2-)). (1)H NMR titrations in CD(3)OD indicated that this receptor is not suitable for recognizing HSO(4)(-) and H(2)PO(4)(-), but weakly binds p-nbz(-), and strongly interacts with ph(2-), dipic(2-), and iph(2-) anions forming 1 : 2 assembled species. The largest beta(2) binding constant was determined for ph(2-), followed by dipic(2-) and finally iph(2-). The effect of the anionic substrates on the electron-transfer process of the ferrocene units of R was evaluated using cyclic voltammetry (CV) and square wave voltammetry (SWV) in methanol solution and 0.1 mol dm(-3)(CH(3))(4)NCl as the supporting electrolyte. Titrations of the receptor were undertaken by addition of anion solutions in their tetrabutylammonium or tetramethylammonium forms. The protonated ligand exhibits a reversible voltammogram, which shifts cathodically in the presence of the substrates. The data revealed kinetic constraints in the formation of the receptor/substrate entity for dipic(2-), ph(2-) and iph(2-) anions, but not for p-nbz(-). In spite of the slow kinetics of assembled species formation with the ph(2-) substrate, this anion provides the largest redox-response when the supramolecular entity is formed, followed by dipic(2-), iph(2-) and finally p-nbz(-) anions. This trend is in agreement with the (1)H NMR results and the values of the binding constants. Single crystal X-ray structures of the receptor with PF(6)(-), ph(2-), iph(2-) and p-nbz(-) were carried out and showed that supermolecules with a RS(2) stoichiometry are formed with the first three anions, but RS(4) with p-nbz(-). In all cases the binding occurs outside the macrocyclic cavity via N-H...O=C hydrogen bonds for carboxylate anions and N-H...F hydrogen bonds for the PF(6)(-) anion, which is in agreement with the solution results. The macrocyclic framework adopts different conformations in order to interact with each substrate having Fe...Fe intramolecular distances ranging from 10.125(14) to 12.783(15)A.

GROMACS: Fast, flexible, and free

This article describes the software suite GROMACS (Groningen MAchine for Chemical Simulation) that was developed at the University of Groningen, The Netherlands, in the early 1990s. The software, written in ANSI C, originates from a parallel hardware project, and is well suited for parallelization on processor clusters. By careful optimization of neighbor searching and of inner loop performance, GROMACS is a very fast program for molecular dynamics simulation. It does not have a force field of its own, but is compatible with GROMOS, OPLS, AMBER, and ENCAD force fields. In addition, it can handle polarizable shell models and flexible constraints. The program is versatile, as force routines can be added by the user, tabulated functions can be specified, and analyses can be easily customized. Nonequilibrium dynamics and free energy determinations are incorporated. Interfaces with popular quantum-chemical packages (MOPAC, GAMES-UK, GAUSSIAN) are provided to perform mixed MM/QM simulations. The package includes about 100 utility and analysis programs. GROMACS is in the public domain and distributed (with source code and documentation) under the GNU General Public License. It is maintained by a group of developers from the Universities of Groningen, Uppsala, and Stockholm, and the Max Planck Institute for Polymer Research in Mainz. Its Web site is http://www.gromacs.org.

Structural heterogeneity of cryotrapped intermediates in the bacterial blue light photoreceptor, photoactive yellow protein

We investigate by X-ray crystallographic techniques the cryotrapped states that accumulate on controlled illumination of the blue light photoreceptor, photoactive yellow protein (PYP), at 110 K in both the wild-type species and its E46Q mutant. These states are related to those that occur during the chromophore isomerization process in the PYP photocycle at room temperature. The structures present in such states were determined at high resolution, 0.95-1.05A. In both wild type and mutant PYP, the cryotrapped state is not composed of a single, quasitransition state structure but rather of a heterogeneous mixture of three species in addition to the ground state structure. We identify and refine these three photoactivated species under the assumption that the structural changes are limited to simple isomerization events of the chromophore that otherwise retains chemical bonding similar to that in the ground state. The refined chromophore models are essentially identical in the wild type and the E46Q mutant, which implies that the early stages of their photocycle mechanisms are the same.

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.

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.

Dynamical transition and proteinquake in photoactive yellow protein

Conformational dynamics in protein functioning covers a wide range of time scales from nanosecond fluctuations around a conformation to the large-amplitude conformational changes of milliseconds or longer. We illustrate a picture of cooperative coupling among such motions of different time scales in a model protein, photoactive yellow protein, by proposing a model that can consistently explain the experimental results on the photocycle of photoactive yellow protein. The model provides a scenario in which the global collective motion induced by the unfolding of the N-terminal domain promotes the loosening of the atomistic packing around the chromophore, which produces the favorable molecular environment for the photoexcited chromophore, thereby stabilizing the partially unfolded intermediate in the photocycle. The proteinquake, the large conformational change triggered by the local structural disturbance, plays a decisive role in controlling the kinetics of functioning.

Resonance Raman analysis of the mechanism of energy storage and chromophore distortion in the primary visual photoproduct

The vibrational structure of the chromophore in the primary photoproduct of vision, bathorhodopsin, is examined to determine the cause of the anomalously decoupled and intense C(11)=C(12) hydrogen-out-of-plane (HOOP) wagging modes and their relation to energy storage in the primary photoproduct. Low-temperature (77 K) resonance Raman spectra of Glu181 and Ser186 mutants of bovine rhodopsin reveal only mild mutagenic perturbations of the photoproduct spectrum suggesting that dipolar, electrostatic, or steric interactions with these residues do not cause the HOOP mode frequencies and intensities. Density functional theory calculations are performed to investigate the effect of geometric distortion on the HOOP coupling. The decoupled HOOP modes can be simulated by imposing approximately 40 degrees twists in the same direction about the C(11)=C(12) and C(12)-C(13) bonds. Sequence comparison and examination of the binding site suggests that these distortions are caused by three constraints consisting of an electrostatic anchor between the protonated Schiff base and the Glu113 counterion, as well as steric interactions of the 9- and 13-methyl groups with surrounding residues. This distortion stores light energy that is used to drive the subsequent protein conformational changes that activate rhodopsin.

Global and target analysis of time-resolved spectra

In biological/bioenergetics research the response of a complex system to an externally applied perturbation is often studied. Spectroscopic measurements at multiple wavelengths are used to monitor the kinetics. These time-resolved spectra are considered as an example of multiway data. In this paper, the methodology for global and target analysis of time-resolved spectra is reviewed. To fully extract the information from the overwhelming amount of data, a model-based analysis is mandatory. This analysis is based upon assumptions regarding the measurement process and upon a physicochemical model for the complex system. This model is composed of building blocks representing scientific knowledge and assumptions. Building blocks are the instrument response function (IRF), the components of the system connected in a kinetic scheme, and anisotropy properties of the components. The combination of a model for the kinetics and for the spectra of the components results in a more powerful spectrotemporal model. The model parameters, like rate constants and spectra, can be estimated from the data, thus providing a concise description of the complex system dynamics. This spectrotemporal modeling approach is illustrated with an elaborate case study of the ultrafast dynamics of the photoactive yellow protein.

Chromophore conformation and the evolution of tertiary structural changes in photoactive yellow protein

We use time-resolved crystallography to observe the structural progression of a bacterial blue light photoreceptor throughout its photocycle. Data were collected from 10 ns to 100 ms after photoactivation of the E46Q mutant of photoactive yellow protein. Refinement of transient chromophore conformations shows that the spectroscopically distinct intermediates are formed via progressive disruption of the hydrogen bond network to the chromophore. Although structural change occurs within a few nanoseconds on and around the chromophore, it takes milliseconds for a distinct pattern of tertiary structural change to fully progress through the entire molecule, thus generating the putative signaling state. Remarkably, the coupling between the chromophore conformation and the tertiary structure of this small protein is not tight: there are leads and lags between changes in the conformation of the chromophore and the protein tertiary structure.

Photoactivation of the photoactive yellow protein: why photon absorption triggers a trans-to-cis Isomerization of the chromophore in the protein

Atomistic QM/MM simulations have been carried out on the complete photocycle of Photoactive Yellow Protein, a bacterial photoreceptor, in which blue light triggers isomerization of a covalently bound chromophore. The "chemical role" of the protein cavity in the control of the photoisomerization step has been elucidated. Isomerization is facilitated due to preferential electrostatic stabilization of the chromophore's excited state by the guanidium group of Arg52, located just above the negatively charged chromophore ring. In vacuo isomerization does not occur. Isomerization of the double bond is enhanced relative to isomerization of a single bond due to the steric interactions between the phenyl ring of the chromophore and the side chains of Arg52 and Phe62. In the isomerized configuration (ground-state cis), a proton transfer from Glu46 to the chromophore is far more probable than in the initial configuration (ground-state trans). It is this proton transfer that initiates the conformational changes within the protein, which are believed to lead to signaling.

Femtosecond broadband stimulated Raman: a new approach for high-performance vibrational spectroscopy

Femtosecond stimulated Raman spectroscopy (FSRS) is a new technique that produces high-quality vibrational spectra free from background fluorescence. FSRS combines a narrow-bandwidth picosecond Raman pump pulse with an approximately 80 fs continuum probe pulse to produce stimulated Raman spectra from the pump-induced gain in the probe spectrum. The high intensity of the Raman pump combined with the broad bandwidth of the probe produces high signal-to-noise vibrational spectra with very short data acquisition times. FSRS spectra of standard solutions and solvents such as aqueous Na2SO4, aqueous KNO3, methanol, isopropanol, and cyclohexane are collected in seconds. Furthermore, stimulated Raman spectra can be obtained using just a single pump-probe pulse pair that illuminates the sample for only approximately 1 ps. Fluorescence rejection is demonstrated by collecting FSRS spectra of dyes (rhodamine 6G, chlorophyll a, and DTTCI) with varying degrees of fluorescence background and resonance enhancement. The high signal-to-noise, short data acquisition time, fluorescence rejection, and high spectral and temporal resolution of femtosecond stimulated Raman spectroscopy make it a valuable new vibrational spectroscopic technique.

Structural basis of a phototropin light switch

Phototropins are light-activated kinases important for plant responses to blue light. Light initiates signaling in these proteins by generating a covalent protein-flavin mononucleotide (FMN) adduct within sensory Per-ARNT-Sim (PAS) domains. We characterized the light-dependent changes of a phototropin PAS domain by solution nuclear magnetic resonance spectroscopy and found that an alpha helix located outside the canonical domain plays a key role in this activation process. Although this helix associates with the PAS core in the dark, photoinduced changes in the domain structure disrupt this interaction. We propose that this mechanism couples light-dependent bond formation to kinase activation and identifies a signaling pathway conserved among PAS domains.

Initial steps of signal generation in photoactive yellow protein revealed with femtosecond mid-infrared spectroscopy

Photoactive yellow protein (PYP) is a bacterial blue light sensor that induces Halorhodospira halophila to swim away from intense blue light. Light absorption by PYP's intrinsic chromophore, p-coumaric acid, leads to the initiation of a photocycle that comprises several distinct intermediates. Here we describe the initial structural changes of the chromophore and its nearby amino acids, using visible pump/mid-infrared probe spectroscopy. Upon photoexcitation, the trans bands of the chromophore are bleached, and shifts of the phenol ring bands occur. The latter are ascribed to charge translocation, which probably plays an essential role in driving the trans to cis isomerization process. We conclude that breaking of the hydrogen bond of the chromophore's C=O group with amino acid Cys69 and formation of a stable cis ground state occur in approximately 2 ps. Dynamic changes also include rearrangements of the hydrogen-bonding network of the amino acids around the chromophore. Relaxation of the coumaryl tail of the chromophore occurs in 0.9-1 ns, which event we identify with the I(0) to I(1) transition observed in visible spectroscopy.

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

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

Light-induced structural changes in the LOV2 domain of Adiantum phytochrome3 studied by low-temperature FTIR and UV-visible spectroscopy

Phototropin (Phot) is a blue-light receptor in plants. The molecule has two FMN (flavin mononucleotide) binding domains named LOV (light-, oxygen-, and voltage-sensing), which is a subset of the PAS (Per-Arnt-Sim) superfamily. Illumination of the phot-LOV domains in the dark state (D447) produces a covalent C(4a) flavin-cysteinyl adduct (S390) via a triplet excited state (L660), which reverts to D447 in the dark. In this work, we studied the light-induced structural changes in the LOV2 domain of Adiantum phytochrome3 (phy3), which is a fusion protein of phot containing the phytochrome chromophoric domain, by low-temperature UV-visible and FTIR spectroscopy. UV-visible spectroscopy detected only one intermediate state, S390, in the temperature range from 77 to 295 K, indicating that the adduct is produced even at temperatures as low as 77 K, although a portion of D447 cannot be converted to S390 at low temperatures possibly because of motional freezing. In the whole temperature range, FTIR spectra in the S-H stretching frequency region showed that Cys966 of phy3-LOV2 is protonated in D447 and unprotonated on illumination, supporting adduct formation. The pK(a) of the S-H group in D447 is estimated to be >10. FTIR spectra also showed the light-induced appearance of a positive peak around 3621 cm(-1) in the whole temperature range, indicating that adduct formation accompanies rearrangement of a hydrogen bond of a water molecule(s), which can be either water25, water45, or both, near the chromophore. In contrast to the weak temperature dependence of the spectral changes in the UV-visible absorption and the FTIR of both S-H and O-H stretching bands, light-induced changes in the amide I vibration that probes protein backbone structure vary significantly with the increase in temperature. The spectral changes suggest that light excitation of FMN loosens the local structure around it, particularly in turns, in the early stages and that another change subsequently takes place to tighten it, mainly in beta-structure, but some occur in the alpha-helical structure of the protein moiety as well. Interestingly, these changes proceed without altering the shape of UV-visible spectra, suggesting the presence of multiple conformation states in S390.

Time-resolved photothermal methods: accessing time-resolved thermodynamics of photoinduced processes in chemistry and biology

Photothermal methods are currently being employed in a variety of research areas, ranging from materials science to environmental monitoring. Despite the common term which they are collected under, the implementations of these techniques are as diverse as the fields of application. In this review, we concentrate on the recent applications of time-resolved methods in photochemistry and photobiology.