New photointermediates in the two photon signaling pathway of sensory rhodopsin-I

Sensory rhodopsin-I (SRI) functions as a color discriminating receptor in halobacterial phototaxis. SRI exists in the membrane as a molecular complex with a signal transducer protein. Excitation of its thermally stable form, SRI(587), generates a long-lived photointermediate of its photocycle, S(373), and an attractant phototactic response. S(373) decays thermally in a few seconds into SRI(587.) However, when S(373) is excited by UV-blue light, it photoconverts into SRI(587) in less than a second, generating a repellent phototactic response. Only one intermediate of this back-photoreaction, S(b)(510), is known. We studied the back-photoreaction in both native SRI and its transducer free form fSRI by measuring laser flash induced absorption changes of S(373) photoproducts from 100 ns to 1 s in the 350-750 nm range. Using global exponential fitting, we determined the spectra and kinetics of the photointermediates. S(373) and fS(373) when pumped with 355 nm laser light generate in less than 100 ns two intermediate species: a previously undetected species that absorbs maximally at about 410 nm, S(b)(410), and the previously described S(b)(510). These two intermediates appear to be in a rapid equilibrium, which probably entails protonation change of the Schiff base chromophore. At pH 6 this system relaxes to SRI(587) via another intermediate absorbing maximally around 550 nm, which thermally decays back to the ground state. The same intermediates are seen in the presence and absence of transducer; however, the kinetics are affected by binding of the transducer.     

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.     

Proton circulation during the photocycle of sensory rhodopsin II.

Sensory rhodopsin II (SRII) in Halobacterium salinarum membranes is a phototaxis receptor that signals through its bound transducer HtrII for avoidance of blue-green light. In the present study we investigated the proton movements during the photocycle of SRII in the HtrII-free and HtrII-complexed form. We monitored sustained light-induced pH changes with a pH electrode, and laser flash-induced pH changes with the pH indicator pyranine using sealed membrane vesicles and open sheets containing the free or the complexed receptor. The results demonstrated that SRII takes up a proton in M-to-O conversion and releases it during O-decay. The uptake and release are from and to the extracellular side, and therefore SRII does not transport the proton across the membrane. The pH dependence of the SRII photocycle indicated the presence of a protonatable group (pK(a) approximately 7.5) in the extracellular proton-conducting path, which plays a role in proton uptake by the Schiff base in the M-to-O conversion. The extracellular proton circulation produced by SRII was not blocked by HtrII complexation, unlike the cytoplasmic proton conduction in SRI that was found in the same series of measurements to be blocked by its transducer, HtrI. The implications of this finding for current models of SRI and SRII signaling are discussed.     

Quantitation of photochromism of sensory rhodopsin-I by computerized tracking of Halobacterium halobium cells

The swimming behavior of Halobacterium halobium is controlled by light which acts through retinal photoreceptor proteins. The sensing of near-ultraviolet (u.v.) was proposed to be mediated by the thermally metastable intermediate SR-I373 that is formed upon orange light absorption by sensory rhodopsin-I (SR-I). In order to test the validity of this proposal, we analyzed the photochromic behavior of the functional near-u.v. receptor in situ by use of an automated cell tracking system. The system was specifically designed for detection of swimming reversals in individual cells and calibrated with a straight-swimming mutant of H. halobium. Quantitative analysis of the response of the cells to near-u.v. revealed that orange background light increased the number of active near-u.v. receptor molecules. The intensity-dependence of this effect fitted into the kinetic scheme of a photochromic receptor pigment. The half-life of the functional near-u.v. receptor species was determined under continuous orange background light and found to be similar to that of the SR-I373 intermediate of sensory rhodopsin-I in intact cells. These results clearly support the assignment of the near-u.v. receptor to SR-I373. The kind of kinetic analysis described here, might be a useful tool in assigning spectroscopic data of pigments to photoreceptor function also in other organisms.     

Functional significance of a protein conformation change at the cytoplasmic end of helix F during the bacteriorhodopsin photocycle.

The second half of the photocycle of the light-driven proton pump bacteriorhodopsin includes proton transfers between D96 and the retinal Schiff base (the M to N reaction) and between the cytoplasmic surface and D96 (decay of the N intermediate). The inhibitory effects of decreased water activity and increased hydrostatic pressure have suggested that a conformational change resulting in greater hydration of the cytoplasmic region is required for proton transfer from D96 to the Schiff base, and have raised the possibility that the reversal of this process might be required for the subsequent reprotonation of D96 from the cytoplasmic surface. Tilt of the cytoplasmic end of helix F has been suggested by electron diffraction of the M intermediate. Introduction of bulky groups, such as various maleimide labels, to engineered cysteines at the cytoplasmic ends of helices A, B, C, E, and G produce only minor perturbation of the decays of M and N, but major changes in these reactions when the label is linked to helix F. In these samples the reprotonation of the Schiff base is accelerated and the reprotonation of D96 is strongly retarded. Cross-linking with benzophenone introduced at this location, but not at the others, causes the opposite change: the reprotonation of the Schiff base is greatly slowed while the reprotonation of D96 is accelerated. We conclude that, consistent with the structure from diffraction, the proton transfers in the second half of the photocycle are facilitated by motion of the cytoplasmic end of helix F, first away from the center of the protein and then back.     

Early structural rearrangements in the photocycle of an integral membrane sensory receptor

Sensory rhodopsins are the primary receptors of vision in animals and phototaxis in microorganisms. Light triggers the rapid isomerization of a buried retinal chromophore, which the protein both accommodates and amplifies into the larger structural rearrangements required for signaling. We trapped an early intermediate of the photocycle of sensory rhodopsin II from Natronobacterium pharaonis (pSRII) in 3D crystals and determined its X-ray structure to 2.3 A resolution. The observed structural rearrangements were localized near the retinal chromophore, with a key water molecule becoming disordered and the retinal's beta-ionone ring undergoing a prominent movement. Comparison with the early structural rearrangements of bacteriorhodopsin illustrates how modifications in the retinal binding pocket of pSRII allow subtle differences in the early relaxation of photoisomerized retinal.     

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.     

The effect of protein conformation change from alpha(II) to alpha(I) on the bacteriorhodopsin photocycle

The bacteriorhodopsin (bR) photocycle was followed by use of time-resolved Fourier-transform infrared (FTIR) spectroscopy as a function of temperature (15-85 degrees C) as the alpha(II) --> alpha(I) conformational transition occurs. The photocycle rate increases with increasing temperature, but its efficiency is found to be drastically reduced as the transition takes place. A large shift is observed in the all-trans left arrow over right arrow 13-cis equilibrium due to the increased stability of the 13-cis isomer in alpha(I) form. This, together with the increase in the rate of dark adaptation as the temperature increases, leads to a large increase in the 13-cis isomer concentration in bR in the alpha(I) form. The fact that 13-cis retinal has a much-reduced absorption cross-section and its inability to pump protons leads to an observed large reduction in the concentration of the observed photocycle intermediates, as well as the proton gradient at a given light intensity. These results suggest that nature might have selected the alpha(II) rather than the alpha(I) form as the helical conformation in bR to stabilize the all-trans retinal isomer that is a better light absorber and is capable of pumping protons.     

Removal of the transducer protein from sensory rhodopsin I exposes sites of proton release and uptake during the receptor photocycle.

The phototaxis receptor sensory rhodopsin-I (SR-I) was genetically truncated in the COOH terminus which leads to overexpression in Halobacterium salinarium and was expressed in the presence and absence of its transducer, HtrI. Pyranine (8-hydroxyl-1,3,6-pyrene-trisulfonate) was used as a pH probe to show that proton release to the bulk phase results from the SR-I587 to S373 photoconversion, but only in the absence of transducer. The stoichiometry is 1 proton/S373 molecule formed. When SR-I is overexpressed in the presence of HtrI, the kinetics of the thermal return of S373 to SR-I587 is biphasic. A kinetic dissection indicates that overexpressed SR-I is present in two pools: one pool which generates an SR-I molecule possessing a normal (i.e., transducer-interacting) pH-independent rate of S373 decay, and a second pool which shows the pH-dependent kinetics of transducer-free S373 decay. The truncated SR-I receptor functions normally based on the following criteria: (i) Truncated SR-I restores phototaxis (attractant and repellent responses) when expressed in a strain lacking native SR-I, but containing HtrI. (ii) The absorption spectrum and the flash-induced absorption difference spectrum are indistinguishable from those of native SR-I. (iii) The rate of decay of S373 is pH-dependent in the absence of HtrI but not in the presence of HtrI. The data presented here indicate that a proton-conducting path exists between the protonated Schiff base nitrogen and the extramembranous environment in the transducer-free receptor, and transducer binding blocks this path.     

Crystallographic analysis of protein conformational changes in the bacteriorhodopsin photocycle

A variety of neutron, X-ray and electron diffraction experiments have established that the transmembrane regions of bacteriorhodopsin undergo significant light-induced changes in conformation during the course of the photocycle. A recent comprehensive electron crystallographic analysis of light-driven structural changes in wild-type bacteriorhodopsin and a number of mutants has established that a single, large protein conformational change occurs within 1 ms after illumination, roughly coincident with the time scale of formation of the M(2) intermediate in the photocycle of wild-type bacteriorhodopsin. Minor differences in structural changes that are observed in mutants that display long-lived M(2), N or O intermediates are best described as variations of one fundamental type of conformational change, rather than representing structural changes that are unique to the optical intermediate that is accumulated. These observations support a model for the photocycle of wild-type bacteriorhodopsin in which the structures of the initial state and the early intermediates (K, L and M(1)) are well approximated by one protein conformation in which the Schiff base has extracellular accessibility, while the structures of the later intermediates (M(2), N and O) are well approximated by the other protein conformation in which the Schiff base has cytoplasmic accessibility.     

Local-global conformational coupling in a heptahelical membrane protein: transport mechanism from crystal structures of the nine states in the bacteriorhodopsin photocycle

Proton pumps utilize a chemical or photochemical reaction to create pH and electrical gradients between the interior and the exterior of cells and organelles that energize ATP synthesis and the accumulation and extrusion of solutes and ions. G-protein coupled receptors bind agonists and assume signaling states that communicate with the coupled transducers. How these two kinds of proteins convert chemical potential to a proton transmembrane electrochemical potential or a signal are the great questions in structural membrane biology, and they may have a common answer. Bacteriorhodopsin, a particularly simple integral membrane protein, functions as a proton pump but has a heptahelical structure like membrane receptors. Crystallographic structures are now available for all of the intermediates of the bacteriorhodopsin transport cycle, and they describe the proton translocation mechanism, step by step and in atomic detail. The results show how local conformational changes propagate upon the gradual relaxation of the initially twisted photoisomerized retinal toward the two membrane surfaces. Such local-global conformational coupling between the ligand-binding site and the distant regions of the protein may be the shared mechanism of ion pumps and G-protein related receptors.     

Identification of rare partially unfolded states in equilibrium with the native conformation in an all beta-barrel protein

Human acidic fibroblast growth factor 1 (hFGF-1) is an all beta-barrel protein, and the secondary structural elements in the protein include 12 antiparallel beta-strands arranged into a beta-trefoil fold. In the present study, we investigate the stability of hFGF-1 by hydrogen-deuterium exchange as a function of urea concentration. Urea-induced equilibrium unfolding of hFGF-1 monitored by fluorescence and CD spectroscopy suggests that the protein unfolds by a two-state (native to denatured) mechanism. Hydrogen exchange in hFGF-1, under the experimental conditions used, occurs by the EX2 mechanism. In contrast to the equilibrium unfolding events monitored by optical probes, native state hydrogen exchange data show that the beta-trefoil architecture of hFGF-1 does not behave as a single cooperative unit. There are at least two structurally independent units with differing stabilities in hFGF-1. Beta-strands I, II, III, VI, VII, X, XI, and XII fit into the global unfolding isotherm. By contrast, residues in beta-strands IV, V, VIII, and IX exchange by the subfolding isotherm and could be responsible for the occurrence of high-energy partially unfolded state(s) in hFGF-1. There appears to be a broad continuum of stabilities among the four beta-strands (beta-strands IV, V, VIII, and IX) constituting the subglobal folding unit. The slow exchanging residues in hFGF-1 do not represent the folding nucleus of the protein.     

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.     

The photochemical reactions of bacterial sensory rhodopsin-I. Flash photolysis study in the one microsecond to eight second time window.

Halobacterium halobium Flx mutants are deficient in bacteriorhodopsin (bR) and halorhodopsin (hR). Such strains are phototactic and the light signal detectors are two additional retinal pigments, sensory rhodopsins I and II (sR-I and sR-II), which absorb maximally at 587 and 480 nm, respectively. A retinal-deficient Flx mutant, Flx5R, overproduces sR-I-opsin and does not show any photochemical activity other than that of sR-I after the pigment is regenerated by addition of all-trans retinal. Using native membrane vesicles from this strain, we have resolved a new photointermediate in the sR-I photocycle between the early bathointermediate S610 and the later intermediate S373. The new form, S560, resembles the L intermediate of bR in its position in the photoreaction cycle, its relatively low extinction, and its moderate blue shift. It forms with a half-time of approximately 90 microseconds at 21 degrees C, concomitant with the decay of S610. Its decay with a half-time of 270 microseconds parallels the appearance of S373. From a data set consisting of laser flash-induced absorbance changes (300 ns, 580-nm excitation) measured at 24 wavelengths from 340 to 720 nm in a time window spanning 1 microsecond to 8 s we have calculated the spectra of the photocycle intermediates assuming a unidirectional, unbranched reaction scheme.     

Conformational changes in the photocycle of Anabaena sensory rhodopsin: absence of the Schiff base counterion protonation signal

Anabaena sensory rhodopsin (ASR) is a novel microbial rhodopsin recently discovered in the freshwater cyanobacterium Anabaena sp. PCC7120. This protein most likely functions as a photosensory receptor as do the related haloarchaeal sensory rhodopsins. However, unlike the archaeal pigments, which are tightly bound to their cognate membrane-embedded transducers, ASR interacts with a soluble cytoplasmic protein analogous to transducers of animal vertebrate rhodopsins. In this study, infrared spectroscopy was used to examine the molecular mechanism of photoactivation in ASR. Light adaptation of the pigment leads to a phototransformation of an all-trans/15-anti to 13-cis/15-syn retinylidene-containing species very similar in chromophore structural changes to those caused by dark adaptation in bacteriorhodopsin. Following 532 nm laser-pulsed excitation, the protein exhibits predominantly an all-trans retinylidene photocycle containing a deprotonated Schiff base species similar to those of other microbial rhodopsins such as bacteriorhodopsin, sensory rhodopsin II, and Neurospora rhodopsin. However, no changes are observed in the Schiff base counterion Asp-75, which remains unprotonated throughout the photocycle. This result along with other evidence indicates that the Schiff base proton release mechanism differs significantly from that of other known microbial rhodopsins, possibly because of the absence of a second carboxylate group at the ASR photoactive site. Several conformational changes are detected during the ASR photocycle including in the transmembrane helices E and G as indicated by hydrogen-bonding alterations of their native cysteine residues. In addition, similarly to animal vertebrate rhodopsin, perturbations of the polar head groups of lipid molecules are detected.     

Electrogenic processes and protein conformational changes accompanying the bacteriorhodopsin photocycle

The possible mechanisms of electrogenic processes accompanying proton transport in bacteriorhodopsin are discussed on the basis of recent structural data of the protein. Apparent inconsistencies between experimental data and their interpretation are considered. Special emphasis is placed on the protein conformational changes accompanying the reprotonation of chromophore and proton uptake stage in the bacteriorhodopsin photocycle.     

Low-temperature heat capacity of DNA in various conformation states

Experimental results are presented on temperature--dependent DNA heat capacity in three different states: a) intact--native DNA in the conformation of double helix, b) disordered conformation of polynucleotide chains in the state of statistical coils, c) completely "degenerated" polynucleotide chains--mechanical mixture of nucleotides. Data on heat capacity (4-400 K) at different water content in the specimens allow a definition of relative changes in the pattern of the entropy temperature dependence for these conformational states with the account for the structural effect of water.     

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.     

Amino acids in the N-terminal region regulate the photocycle of photoactive yellow protein.

The spectroscopic properties of photoactive yellow protein (PYP) partially digested by chymotrypsin were studied. Chymotrypsin yielded three major products that were yellow but distinguishable by SDS-PAGE. They were readily separated by DEAE-Sepharose column chromatography. Protein sequencing and mass spectrometry demonstrated that chymotrypsin cleaved the N-terminal 6, 15, or 23 amino acids (T6, T15, and T23). The blue-shifts of the absorption maxima and the increases in the apparent pK(a) of the chromophores relative to those of intact PYP were less than 4 nm and 0.2, respectively. The absorption spectra of the near-UV intermediates produced from T6, T15, and T23 were identical to that of intact PYP, but with lifetimes that were 140, 2,300, and 4,500 times longer, respectively. These observations suggest that the recovery of the dark state of PYP from the near-UV intermediate is accelerated by the N-terminal region, and that this region acts as a regulatory factor for the photocycle of PYP.     

Brain states: top-down influences in sensory processing

All cortical and thalamic levels of sensory processing are subject to powerful top-down influences, the shaping of lower-level processes by more complex information. New findings on the diversity of top-down interactions show that cortical areas function as adaptive processors, being subject to attention, expectation, and perceptual task. Brain states are determined by the interactions between multiple cortical areas and the modulation of intrinsic circuits by feedback connections. In perceptual learning, both the encoding and recall of learned information involves a selection of the appropriate inputs that convey information about the stimulus being discriminated. Disruption of this interaction may lead to behavioral disorders, including schizophrenia.