Application of FTIR Spectroscopy to the Investigation of Dark Structures and Photoreactions of Visual Pigments

Development and maintenance of vision's first synapse

Synapses in the outer retina are the first information relay points in vision. Here, photoreceptors form synapses onto two types of interneurons, bipolar cells and horizontal cells. Because outer retina synapses are particularly large and highly ordered, they have been a useful system for the discovery of mechanisms underlying synapse specificity and maintenance. Understanding these processes is critical to efforts aimed at restoring visual function through repairing or replacing neurons and promoting their connectivity. We review outer retina neuron synapse architecture, neural migration modes, and the cellular and molecular pathways that play key roles in the development and maintenance of these connections. We further discuss how these mechanisms may impact connectivity in the retina.

Infrared Difference Spectroscopy of Proteins: From Bands to Bonds

Infrared difference spectroscopy probes vibrational changes of proteins upon their perturbation. Compared with other spectroscopic methods, it stands out by its sensitivity to the protonation state, H-bonding, and the conformation of different groups in proteins, including the peptide backbone, amino acid side chains, internal water molecules, or cofactors. In particular, the detection of protonation and H-bonding changes in a time-resolved manner, not easily obtained by other techniques, is one of the most successful applications of IR difference spectroscopy. The present review deals with the use of perturbations designed to specifically change the protein between two (or more) functionally relevant states, a strategy often referred to as reaction-induced IR difference spectroscopy. In the first half of this contribution, I review the technique of reaction-induced IR difference spectroscopy of proteins, with special emphasis given to the preparation of suitable samples and their characterization, strategies for the perturbation of proteins, and methodologies for time-resolved measurements (from nanoseconds to minutes). The second half of this contribution focuses on the spectral interpretation. It starts by reviewing how changes in H-bonding, medium polarity, and vibrational coupling affect vibrational frequencies, intensities, and bandwidths. It is followed by band assignments, a crucial aspect mostly performed with the help of isotopic labeling and site-directed mutagenesis, and complemented by integration and interpretation of the results in the context of the studied protein, an aspect increasingly supported by spectral calculations. Selected examples from the literature, predominately but not exclusively from retinal proteins, are used to illustrate the topics covered in this review.

Féry Infrared Spectrometer for Single-Shot Analysis of Protein Dynamics

Current submillisecond time-resolved broad-band infrared spectroscopy, one of the most frequently used techniques for studying structure-function relationships in life sciences, is typically limited to fast-cycling reactions that can be repeated thousands of times with high frequency. Notably, a majority of chemical and biological processes do not comply with this requirement. For example, the activation of vertebrate rhodopsin, a prototype of many protein receptors in biological organisms that mediate basic functions of life, including vision, smell, and taste, is irreversible. Here we present a dispersive single-shot Féry spectrometer setup that extends such spectroscopy to irreversible and slow-cycling systems by exploiting the unique properties of brilliant synchrotron infrared light combined with an advanced focal plane detector array embedded in a dispersive optical concept. We demonstrate our single-shot method on microbial actinorhodopsin with a slow photocycle and on vertebrate rhodopsin with irreversible activation.

The Two-Photon Reversible Reaction of the Bistable Jumping Spider Rhodopsin-1

Bistable opsins are photopigments expressed in both invertebrates and vertebrates. These light-sensitive G-protein-coupled receptors undergo a reversible reaction upon illumination. A first photon initiates the cis to trans isomerization of the retinal chromophore—attached to the protein through a protonated Schiff base—and a series of transition states that eventually results in the formation of the thermally stable and active Meta state. Excitation by a second photon reverts this process to recover the original ground state. On the other hand, monostable opsins (e.g., bovine rhodopsin) lose their chromophore during the decay of the Meta II state (i.e., they bleach). Spectroscopic studies on the molecular details of the two-photon cycle in bistable opsins are limited. Here, we describe the successful expression and purification of recombinant rhodopsin-1 from the jumping spider Hasarius adansoni (JSR1). In its natural configuration, spectroscopic characterization of JSR1 is hampered by the similar absorption spectra in the visible spectrum of the inactive and active states. We solved this issue by separating their absorption spectra by replacing the endogenous 11-cis retinal chromophore with the blue-shifted 9-cis JSiR1. With this system, we used time-resolved ultraviolet-visible spectroscopy after pulsed laser excitation to obtain kinetic details of the rise and decay of the photocycle intermediates. We also used resonance Raman spectroscopy to elucidate structural changes of the retinal chromophore upon illumination. Our data clearly indicate that the protonated Schiff base is stable throughout the entire photoreaction. We additionally show that the accompanying conformational changes in the protein are different from those of monostable rhodopsin, as recorded by light-induced FTIR difference spectroscopy. Thus, we envisage JSR1 as becoming a model system for future studies on the reaction mechanisms of bistable opsins, e.g., by time-resolved x-ray crystallography.

The arrestin-1 finger loop interacts with two distinct conformations of active rhodopsin

Signaling of the prototypical G protein-coupled receptor (GPCR) rhodopsin through its cognate G protein transducin (G_t) is quenched when arrestin binds to the activated receptor. Although the overall architecture of the rhodopsin/arrestin complex is known, many questions regarding its specificity remain unresolved. Here, using FTIR difference spectroscopy and a dual pH/peptide titration assay, we show that rhodopsin maintains certain flexibility upon binding the "finger loop" of visual arrestin (prepared as synthetic peptide ArrFL-1). We found that two distinct complexes can be stabilized depending on the protonation state of E3.49 in the conserved (D)ERY motif. Both complexes exhibit different interaction modes and affinities of ArrFL-1 binding. The plasticity of the receptor within the rhodopsin/ArrFL-1 complex stands in contrast to the complex with the C terminus of the G_t α-subunit (GαCT), which stabilizes only one specific substate out of the conformational ensemble. However, G_t α-subunit binding and both ArrFL-1-binding modes involve a direct interaction to conserved R3.50, as determined by site-directed mutagenesis. Our findings highlight the importance of receptor conformational flexibility and cytoplasmic proton uptake for modulation of rhodopsin signaling and thereby extend the picture provided by crystal structures of the rhodopsin/arrestin and rhodopsin/ArrFL-1 complexes. Furthermore, the two binding modes of ArrFL-1 identified here involve motifs of conserved amino acids, which indicates that our results may have elucidated a common modulation mechanism of class A GPCR-G protein/-arrestin signaling.

The Activation Pathway of Human Rhodopsin in Comparison to Bovine Rhodopsin

Rhodopsin, the photoreceptor of rod cells, absorbs light to mediate the first step of vision by activating the G protein transducin (Gt). Several human diseases, such as retinitis pigmentosa or congenital night blindness, are linked to rhodopsin malfunctions. Most of the corresponding in vivo studies and structure-function analyses (e.g. based on protein x-ray crystallography or spectroscopy) have been carried out on murine or bovine rhodopsin. Because these rhodopsins differ at several amino acid positions from human rhodopsin, we conducted a comprehensive spectroscopic characterization of human rhodopsin in combination with molecular dynamics simulations. We show by FTIR and UV-visible difference spectroscopy that the light-induced transformations of the early photointermediates are very similar. Significant differences between the pigments appear with formation of the still inactive Meta I state and the transition to active Meta II. However, the conformation of Meta II and its activity toward the G protein are essentially the same, presumably reflecting the evolutionary pressure under which the active state has developed. Altogether, our results show that although the basic activation pathways of human and bovine rhodopsin are similar, structural deviations exist in the inactive conformation and during receptor activation, even between closely related rhodopsins. These differences between the well studied bovine or murine rhodopsins and human rhodopsin have to be taken into account when the influence of point mutations on the activation pathway of human rhodopsin are investigated using the bovine or murine rhodopsin template sequences.

Formation and decay of the arrestin·rhodopsin complex in native disc membranes

In the G protein-coupled receptor rhodopsin, light-induced cis/trans isomerization of the retinal ligand triggers a series of distinct receptor states culminating in the active Metarhodopsin II (Meta II) state, which binds and activates the G protein transducin (Gt). Long before Meta II decays into the aporeceptor opsin and free all-trans-retinal, its signaling is quenched by receptor phosphorylation and binding of the protein arrestin-1, which blocks further access of Gt to Meta II. Although recent crystal structures of arrestin indicate how it might look in a precomplex with the phosphorylated receptor, the transition into the high affinity complex is not understood. Here we applied Fourier transform infrared spectroscopy to monitor the interaction of arrestin-1 and phosphorylated rhodopsin in native disc membranes. By isolating the unique infrared signature of arrestin binding, we directly observed the structural alterations in both reaction partners. In the high affinity complex, rhodopsin adopts a structure similar to Gt-bound Meta II. In arrestin, a modest loss of β-sheet structure indicates an increase in flexibility but is inconsistent with a large scale structural change. During Meta II decay, the arrestin-rhodopsin stoichiometry shifts from 1:1 to 1:2. Arrestin stabilizes half of the receptor population in a specific Meta II protein conformation, whereas the other half decays to inactive opsin. Altogether these results illustrate the distinct binding modes used by arrestin to interact with different functional forms of the receptor.

IR and X-ray time-resolved simultaneous experiments: an opportunity to investigate the dynamics of complex systems and non-equilibrium phenomena using third-generation synchrotron radiation sources

Third-generation storage rings are modern facilities working with high currents and designed to host powerful radiation sources, like undulators and wigglers, and to deliver high-brilliance beams to users. Many experiments at high spatial resolution, such as spectromicroscopy at the nanometre scale and with high temporal resolution to investigate kinetics down to the picosecond regime, are now possible. The next frontier is certainly the combination of different methods in a unique set-up with the ultimate available spatial and temporal resolutions. In the last decade much synchrotron-based research has exploited the advantage of complementary information provided by time-resolved X-ray techniques and optical methods in the UV/Vis and IR domains. New time-resolved and concurrent approaches are necessary to characterize complex systems where physical-chemical phenomena occur under the same experimental conditions, for example to detect kinetic intermediates via complementary but independent observations. In this contribution we present scientific cases from original works and literature reviews to support the proposed IR/X-ray simultaneous approach, with both probes exploiting synchrotron radiation sources. In addition, simple experimental layouts that may take advantage of the high brilliance and the wide spectral distribution of the synchrotron radiation emission will be given for specific researches or applications to investigate dynamic processes and non-equilibrium phenomena occurring in many condensed matter and biological systems, of great interest for both fundamental research and technological applications.

Crystal structure of metarhodopsin II

G-protein-coupled receptors (GPCRs) are seven transmembrane helix (TM) proteins that transduce signals into living cells by binding extracellular ligands and coupling to intracellular heterotrimeric G proteins (Gαβγ). The photoreceptor rhodopsin couples to transducin and bears its ligand 11-cis-retinal covalently bound via a protonated Schiff base to the opsin apoprotein. Absorption of a photon causes retinal cis/trans isomerization and generates the agonist all-trans-retinal in situ. After early photoproducts, the active G-protein-binding intermediate metarhodopsin II (Meta II) is formed, in which the retinal Schiff base is still intact but deprotonated. Dissociation of the proton from the Schiff base breaks a major constraint in the protein and enables further activating steps, including an outward tilt of TM6 and formation of a large cytoplasmic crevice for uptake of the interacting C terminus of the Gα subunit. Owing to Schiff base hydrolysis, Meta II is short-lived and notoriously difficult to crystallize. We therefore soaked opsin crystals with all-trans-retinal to form Meta II, presuming that the crystal's high concentration of opsin in an active conformation (Ops*) may facilitate all-trans-retinal uptake and Schiff base formation. Here we present the 3.0 Å and 2.85 Å crystal structures, respectively, of Meta II alone or in complex with an 11-amino-acid C-terminal fragment derived from Gα (GαCT2). GαCT2 binds in a large crevice at the cytoplasmic side, akin to the binding of a similar Gα-derived peptide to Ops* (ref. 7). In the Meta II structures, the electron density from the retinal ligand seamlessly continues into the Lys 296 side chain, reflecting proper formation of the Schiff base linkage. The retinal is in a relaxed conformation and almost undistorted compared with pure crystalline all-trans-retinal. By comparison with early photoproducts we propose how retinal translocation and rotation induce the gross conformational changes characteristic for Meta II. The structures can now serve as models for the large GPCR family.

FTIR study of the photoreaction of bovine rhodopsin in the presence of hydroxylamine

In bovine rhodopsin, 11-cis-retinal forms a Schiff base linkage with Lys296. The Schiff base is not reactive to hydroxylamine in the dark, which is consistent with the well-protected retinal binding site. In contrast, under illumination it easily forms all-trans retinal oxime, resulting in the loss of color. This suggests that activation of rhodopsin creates a specific reaction channel for hydroxylamine or loosens the chromophore binding pocket. In the present study, to extract structural information on the Schiff base vicinity and to understand the changes upon activation of rhodopsin, we compared light-induced FTIR difference spectra of bovine rhodopsin in the presence and absence of hydroxylamine under physiological pH (approximately 7). Although the previous FTIR study did not observe the complex formation between rhodopsin and G-protein transducin in hydrated films, the present study clearly shows that hydrated films can be used for studies of the interaction between rhodopsin and hydroxylamine. Hydroxylamine does not react with the Schiff base of Meta-I intermediate trapped at 240 K, possibly because of decreased conformational motions under the frozen environment, while FTIR spectroscopy showed that hydroxylamine affects the hydrogen bonds of the Schiff base and water molecules in Meta-I. In contrast, formation of the retinal oxime was clearly observed at 280 K, the characteristic temperature of Meta-II accumulation in the absence of hydroxylamine, and time-dependent formation of retinal oxime was observed from Meta-II at 265 K as well. The obtained difference FTIR spectra of retinal oxime and opsin are different from that of Meta-II. It is likely that the antiparallel beta-sheet constituting a part of the retinal binding pocket at the extracellular surface is structurally disrupted in the presence of hydroxylamine, which allows the hydrolysis of the Schiff base into retinal oxime.

The branched photocycle of the slow-cycling channelrhodopsin-2 mutant C128T

Channelrhodopsins (ChRs) of green algae such as Chlamydomonas are used as neuroscience tools to specifically depolarize cells with light. A crude model of the ChR2 photocycle has been recently established, but details of the photoreactions are widely unknown. Here, we present the photoreactions of a slow-cycling ChR2 mutant (step function rhodopsin), with C128 replaced by threonine and 200-fold extended lifetime of the conducting-state P520. At a late state of the photocycle, a fraction of the proteins branches off into an inactive species, P380, which accumulates during prolonged illumination. At neutral pH, P380 is converted into P353, a species with a characteristic fine-structured spectrum that is interpreted as retroretinyl chromophore. The described branching reactions should be considered, when ChR is used as a neuroscience tool, especially in the case of fluorescence imaging at high light intensities.

New Insights into Light-Induced Deactivation of Active Rhodopsin by SVD and Global Analysis of Time-Resolved UV/Vis- and FTIR-Data

Time-resolved Fourier transform infrared (FTIR) and UV/Vis difference spectra of light induced deactivation of the photoreceptor rhodopsin were simultaneously recorded on the same sample. The data were analyzed by a special designed combination of singular value decomposition and Global analysis to verify our recently published model of receptor deactivation. This mathematical approach enables us to obtain the pure difference spectra of the conversions between the species involved. We found two different species, which could be identified as key intermediates of the model. The new data allow deeper insights into the structural changes that come along with the formation of the deactivated state. By means of this method we can now separate and assign even strongly overlapping and highly coupled bands of the infrared difference spectra.

Retinal dynamics during light activation of rhodopsin revealed by solid-state NMR spectroscopy

Rhodopsin is a canonical member of class A of the G protein-coupled receptors (GPCRs) that are implicated in many of the drug interventions in humans and are of great pharmaceutical interest. The molecular mechanism of rhodopsin activation remains unknown as atomistic structural information for the active metarhodopsin II state is currently lacking. Solid-state (2)H NMR constitutes a powerful approach to study atomic-level dynamics of membrane proteins. In the present application, we describe how information is obtained about interactions of the retinal cofactor with rhodopsin that change with light activation of the photoreceptor. The retinal methyl groups play an important role in rhodopsin function by directing conformational changes upon transition into the active state. Site-specific (2)H labels have been introduced into the methyl groups of retinal and solid-state (2)H NMR methods applied to obtain order parameters and correlation times that quantify the mobility of the cofactor in the inactive dark state, as well as the cryotrapped metarhodopsin I and metarhodopsin II states. Analysis of the angular-dependent (2)H NMR line shapes for selectively deuterated methyl groups of rhodopsin in aligned membranes enables determination of the average ligand conformation within the binding pocket. The relaxation data suggest that the beta-ionone ring is not expelled from its hydrophobic pocket in the transition from the pre-activated metarhodopsin I to the active metarhodopsin II state. Rather, the major structural changes of the retinal cofactor occur already at the metarhodopsin I state in the activation process. The metarhodopsin I to metarhodopsin II transition involves mainly conformational changes of the protein within the membrane lipid bilayer rather than the ligand. The dynamics of the retinylidene methyl groups upon isomerization are explained by an activation mechanism involving cooperative rearrangements of extracellular loop E2 together with transmembrane helices H5 and H6. These activating movements are triggered by steric clashes of the isomerized all-trans retinal with the beta4 strand of the E2 loop and the side chains of Glu(122) and Trp(265) within the binding pocket. The solid-state (2)H NMR data are discussed with regard to the pathway of the energy flow in the receptor activation mechanism.

Monitoring light-induced structural changes of Channelrhodopsin-2 by UV-visible and Fourier transform infrared spectroscopy

Channelrhodopsin-2 (ChR2) is a microbial type rhodopsin and a light-gated cation channel that controls phototaxis in Chlamydomonas. We expressed ChR2 in COS-cells, purified it, and subsequently investigated this unusual photoreceptor by flash photolysis and UV-visible and Fourier transform infrared difference spectroscopy. Several transient photoproducts of the wild type ChR2 were identified, and their kinetics and molecular properties were compared with those of the ChR2 mutant E90Q. Based on the spectroscopic data we developed a model of the photocycle comprising six distinguishable intermediates. This photocycle shows similarities to the photocycle of the ChR2-related Channelrhodopsin of Volvox but also displays significant differences. We show that molecular changes include retinal isomerization, changes in hydrogen bonding of carboxylic acids, and large alterations of the protein backbone structure. These alterations are stronger than those observed in the photocycle of other microbial rhodopsins like bacteriorhodopsin and are related to those occurring in animal rhodopsins. UV-visible and Fourier transform infrared difference spectroscopy revealed two late intermediates with different time constants of tau = 6 and 40 s that exist during the recovery of the dark state. The carboxylic side chain of Glu(90) is involved in the slow transition. The molecular changes during the ChR2 photocycle are discussed with respect to other members of the rhodopsin family.

Structural analysis and dynamics of retinal chromophore in dark and meta I states of rhodopsin from 2H NMR of aligned membranes

Rhodopsin is a prototype for G protein-coupled receptors (GPCRs) that are implicated in many biological responses in humans. A site-directed (2)H NMR approach was used for structural analysis of retinal within its binding cavity in the dark and pre-activated meta I states. Retinal was labeled with (2)H at the C5, C9, or C13 methyl groups by total synthesis, and was used to regenerate the opsin apoprotein. Solid-state (2)H NMR spectra were acquired for aligned membranes in the low-temperature lipid gel phase versus the tilt angle to the magnetic field. Data reduction assumed a static uniaxial distribution, and gave the retinylidene methyl bond orientations plus the alignment disorder (mosaic spread). The dark-state (2)H NMR structure of 11-cis-retinal shows torsional twisting of the polyene chain and the beta-ionone ring. The ligand undergoes restricted motion, as evinced by order parameters of approximately 0.9 for the spinning C-C(2)H(3) groups, with off-axial fluctuations of approximately 15 degrees . Retinal is accommodated within the rhodopsin binding pocket with a negative pre-twist about the C11=C12 double bond that explains its rapid photochemistry and the trajectory of 11-cis to trans isomerization. In the cryo-trapped meta I state, the (2)H NMR structure shows a reduction of the polyene strain, while torsional twisting of the beta-ionone ring is maintained. Distortion of the retinal conformation is interpreted through substituent control of receptor activation. Steric hindrance between trans retinal and Trp265 can trigger formation of the subsequent activated meta II state. Our results are pertinent to quantum and molecular mechanics simulations of ligands bound to GPCRs, and illustrate how (2)H NMR can be applied to study their biological mechanisms of action.

Deactivation and proton transfer in light-induced metarhodopsin II/metarhodopsin III conversion: a time-resolved fourier transform infrared spectroscopic study

Vertebrate rhodopsin shares with other retinal proteins the 11-cis-retinal chromophore and the light-induced 11-cis/trans isomerization triggering its activation pathway. However, only in rhodopsin the retinylidene Schiff base bond to the apoprotein is eventually hydrolyzed, making a complex regeneration pathway necessary. Metabolic regeneration cannot be short-cut, and light absorption in the active metarhodopsin (Meta) II intermediate causes anti/syn isomerization around the retinylidene linkage rather than reversed trans/cis isomerization. A new deactivating pathway is thereby triggered, which ends in the Meta III "retinal storage" product. Using time-resolved Fourier transform infrared spectroscopy, we show that the identified steps of receptor activation, including Schiff base deprotonation, protein structural changes, and proton uptake by the apoprotein, are all reversed. However, Schiff base reprotonation is much faster than the activating deprotonation, whereas the protein structural changes are slower. The final proton release occurs with pK approximately 4.5, similar to the pK of a free Glu residue and to the pK at which the isolated opsin apoprotein becomes active. A forced deprotonation, equivalent to the forced protonation in the activating pathway, which occurs against the unfavorable pH of the medium, is not observed. This explains properties of the final Meta III product, which displays much higher residual activity and is less stable than rhodopsin arising from regeneration with 11-cis-retinal. We propose that the anti/syn conversion can only induce a fast reorientation and distance change of the Schiff base but fails to build up the full set of dark ground state constraints, presumably involving the Glu(134)/Arg(135) cluster.

The all-trans-15-syn-retinal chromophore of metarhodopsin III is a partial agonist and not an inverse agonist

Meta III is formed during the decay of rhodopsin's active receptor state at neutral to alkaline pH by thermal isomerization of the retinal Schiff base C15=N bond, converting the ligand from all-trans 15-anti to all-trans 15-syn. The thereby induced change of ligand geometry switches the receptor to an inactive conformation, such that the decay pathway to Meta III contributes to the deactivation of the signaling state at higher pH values. We have examined the conformation of Meta III over a wider pH range and found that Meta III exists in a pH-dependent conformational equilibrium between this inactive conformation at neutral to alkaline pH and an active conformation similar to that of Meta II, which, however, is assumed at very acidic pH only. The apparent pKa of this transition is around 5.1 and thus several units lower than that of the Meta I/Meta II photoproduct equilibrium with its all-trans 15-anti ligand, but still about 1 unit higher than that of the opsin conformational equilibrium in the absence of ligand. The all-trans-15-syn-retinal chromophore is therefore not an inverse agonist like 11-cis- or 9-cis-retinal, which lock the receptor in an inactive conformation, but a classical partial agonist, which is capable of activating the receptor, yet with an efficiency considerably lower than the full agonist all-trans 15-anti. As the Meta III chromophore differs structurally from this full agonist only in the isomeric state of the C15=N bond, this ligand represents an excellent model system to study principal mechanisms of partial agonism which are helpful to understand the partial agonist behavior of other ligands.

Time-resolved rapid-scan Fourier transform infrared difference spectroscopy on a noncyclic photosystem: rhodopsin photointermediates from Lumi to Meta II

The visual pigment rhodopsin has been extensively studied for the kinetics of its photointermediates by various spectroscopic methods. Unlike such archaeal retinal proteins as bacteriorhodopsin, visual rhodopsin does not thermally recover its dark state after photoexcitation, which precludes repeated excitation of a single sample and thereby complicates time-resolved experiments. Kinetic data on the late rhodopsin photointermediates have so far been available mainly from time-resolved ultraviolet (UV)-visible spectroscopy, but not from Fourier transform infrared (FTIR) spectroscopy. The latter has the advantage of being informative of structural changes of both chromophore and protein, but does not allow the highly reproducible, automated sample exchange procedures available to UV-visible spectroscopy. Using rapid-scan FTIR difference spectroscopy, we obtained time-resolved data sets that were analyzed by a maximum entropy inverse Laplace-transform. Covering the time range from 8 ms to 15 s at temperatures of 0 and -7 degrees C, the transitions from the Lumi to the Meta I and from the Meta I to the Meta II photoproduct states could be resolved. In the transition from Meta I to Meta II, our data reveal a partial deprotonation of the retinal Schiff base preceding the conformational change of the receptor protein to Meta II. The technique and the results are discussed in regard to its advantages as well as its limitations.

The role of Glu181 in the photoactivation of rhodopsin

The visual pigment rhodopsin is a prototypical seven transmembrane helical G protein-coupled receptor. Photoisomerization of its protonated Schiff base (PSB) retinylidene chromophore initiates a progression of metastable intermediates. We studied the structural dynamics of receptor activation by FTIR spectroscopy of recombinant pigments. Formation of the active state, Meta II, is characterized by neutralization of the PSB and its counterion Glu113. We focused on testing the hypothesis of a PSB counterion switch from Glu113 to Glu181 during the transition of rhodopsin to the still inactive Meta I photointermediate. Our results, especially from studies of the E181Q mutant, support the view that both Glu113 and Glu181 are deprotonated, forming a complex counterion to the PSB in rhodopsin, and that the function of the primary counterion shifts from Glu113 to Glu181 during the transition to Meta I. The Meta I conformation in the E181Q mutant is less constrained compared with that of wild-type Meta I. In particular, the hydrogen bonded network linking transmembrane helices 1, 2, and 7, adopts a conformation that is already Meta II-like, while other parts of the receptor appear to be in a Meta I-like conformation similar to wild-type. We conclude that Glu181 is responsible, in part, for controlling the extraordinary high pK(a) of the chromophore PSB in the dark state, which very likely decreases upon transition to Meta I in a stepwise weakening of the interaction between PSB and its complex counterion during the course of receptor activation. A model for the specific role in coupling chromophore isomerization to protein conformational changes concomitant with receptor activation is presented.

Partial agonism in a G Protein-coupled receptor: role of the retinal ring structure in rhodopsin activation

The visual process in rod cells is initiated by absorption of a photon in the rhodopsin retinal chromophore and consequent retinal cis/trans-isomerization. The ring structure of retinal is thought to be needed to transmit the photonic energy into conformational changes culminating in the active metarhodopsin II (Meta II) intermediate. Here, we demonstrate that cis-acyclic retinals, lacking four carbon atoms of the ring, can activate rhodopsin. Detailed analysis of the activation pathway showed that, although the photoproduct pathway is more complex, Meta II formed with almost normal kinetics. However, lack of the ring structure resulted in a low amount of Meta II and a fast decay of activity. We conclude that the main role of the ring structure is to maintain the active state, thus specifying a mechanism of activation by a partial agonist of the G protein-coupled receptor rhodopsin.

Deuterium NMR structure of retinal in the ground state of rhodopsin

The conformation of retinal bound to the G protein-coupled receptor rhodopsin is intimately linked to its photochemistry, which initiates the visual process. Site-directed deuterium ((2)H) NMR spectroscopy was used to investigate the structure of retinal within the binding pocket of bovine rhodopsin. Aligned recombinant membranes were studied containing rhodopsin that was regenerated with retinal (2)H-labeled at the C(5), C(9), or C(13) methyl groups by total synthesis. Studies were conducted at temperatures below the gel to liquid-crystalline phase transition of the membrane lipid bilayer, where rotational and translational diffusion of rhodopsin is effectively quenched. The experimental tilt series of (2)H NMR spectra were fit to a theoretical line shape analysis [Nevzorov, A. A., Moltke, S., Heyn, M. P., and Brown, M. F. (1999) J. Am. Chem. Soc. 121, 7636-7643] giving the retinylidene bond orientations with respect to the membrane normal in the dark state. Moreover, the relative orientations of pairs of methyl groups were used to calculate effective torsional angles between different planes of unsaturation of the retinal chromophore. Our results are consistent with significant conformational distortion of retinal, and they have important implications for quantum mechanical calculations of its electronic spectral properties. In particular, we find that the beta-ionone ring has a twisted 6-s-cis conformation, whereas the polyene chain is twisted 12-s-trans. The conformational strain of retinal as revealed by solid-state (2)H NMR is significant for explaining the quantum yields and mechanism of its ultrafast photoisomerization in visual pigments. This work provides a consensus view of the retinal conformation in rhodopsin as seen by X-ray diffraction, solid-state NMR spectroscopy, and quantum chemical calculations.

Transition of Rhodopsin into the Active Metarhodopsin II State Opens a New Light-induced Pathway Linked to Schiff Base Isomerization

Rhodopsin bears 11-cis-retinal covalently bound by a protonated Schiff base linkage. 11-cis/all-trans isomerization, induced by absorption of green light, leads to active metarhodopsin II, in which the Schiff base is intact but deprotonated. The subsequent metabolic retinoid cycle starts with Schiff base hydrolysis and release of photolyzed all-trans-retinal from the active site and ends with the uptake of fresh 11-cis-retinal. To probe chromophore-protein interaction in the active state, we have studied the effects of blue light absorption on metarhodopsin II using infrared and time-resolved UV-visible spectroscopy. A light-induced shortcut of the retinoid cycle, as it occurs in other retinal proteins, is not observed. The predominantly formed illumination product contains all-trans-retinal, although the spectra reflect Schiff base reprotonation and protein deactivation. By its kinetics of formation and decay, its low temperature photointermediates, and its interaction with transducin, this illumination product is identified as metarhodopsin III. This species is known to bind all-trans-retinal via a reprotonated Schiff base and forms normally in parallel to retinal release. We find that its generation by light absorption is only achieved when starting from active metarhodopsin II and is not found with any of its precursors, including metarhodopsin I. Based on the finding of others that metarhodopsin III binds retinal in all-trans-C(15)-syn configuration, we can now conclude that light-induced formation of metarhodopsin III operates by Schiff base isomerization ("second switch"). Our reaction model assumes steric hindrance of the retinal polyene chain in the active conformation, thus preventing central double bond isomerization.

Constraints of the 9-Methyl Group Binding Pocket of the Rhodopsin Chromophore Probed by 9-Halogeno Substitution

Sterical constraints of the 9-methyl-binding pocket of the rhodopsin chromophore are probed using retinal analogues carrying substituents of increasing size at the 9 position (H, F, Cl, Br, CH(3), and I). The corresponding 11-Z retinals were employed to investigate formation of photosensitive pigment, and the primary photoproduct was identified by Fourier transform infrared difference spectroscopy. In addition, any effects of cumulative strain were studied by introduction of the 9-Z configuration and/or the alpha-retinal ring structure. Our results show that the 9-F analogue still can escape from the 9-methyl-binding pocket and that its photochemistry behaves very similar to the 9-demethyl analogue. The 9-Cl and 9-Br analogues behave very similar to the native 9-methyl pigments, but the 9-I retinal does not fit very well and shows poor pigment formation. This puts an upper limit on the radial dimension of the 9-methyl pocket at 0.45-0.50 nm. Introduction of the alpha-retinal ring constraint in the 11-Z series results in cumulative strain, because the 9-I and 9-Br derivatives cannot bind to generate a photopigment. The 9-Z configuration can partially compensate for the additional alpha-retinal strain. The corresponding 9-Br analogue does form a photopigment, and the other derivatives give increased photopigment yields compared to the corresponding 11-Z derivatives. In fact, 9-Z-alpha-retinal would be an interesting candidate for retinal supplementation studies. Our data provide direct support for the concept that the 9-methyl group is an important determinant in ligand anchoring and activation of the protein and in general agree with a three-point interaction model involving the ring, 9-methyl group, and aldehyde function.

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.

Acid-base equilibria in rhodopsin: dependence of the protonation state of glu134 on its environment

Glutamic acid E134 in rhodopsin is part of a highly conserved triad, D(E)RY, located near the cytoplasmic lipid/water interface in transmembrane helix 3 of G protein-coupled receptors (GPCRs). A large body of experimental evidence suggests that the protonation of E134 plays a role in the mechanism of activation of rhodopsin and other GPCRs as well. For E134 to change its protonation state, its pK(a) value must shift from values below physiological pH to higher values. Because of the proximity of the triad to the lipid/water interface, it was hypothesized that a change in solvent around E134 from water to lipid could induce such a shift in pK(a). To test this hypothesis, the pK(a) values of the titratable amino acid residues in rhodopsin have been calculated and the change in solvent around E134 was modeled by shifting the position of the lipid/water interface. The approach used to carry out the pK(a) calculations takes into account the partial immersion of transmembrane proteins in lipid. Qualitative experimental evidence is available for several residues regarding their likely protonation state in rhodopsin at or near physiological pH. Comparison of the calculated pK(a) values with these experimental findings shows good agreement between the two. Notably, glutamic acids E122 and E181 were found to be protonated. The pK(a) values were then calculated for a range of lipid/water interface positions. Although the surrounding solvent of several titratable residues changed from water to lipid in this range, leading to pK(a) shifts in most cases, only for E134 would the shift lead to a change in protonation state at physiological pH. Thus, our results show that the protonation state of E134 is particularly sensitive to its environment. This sensitivity together with the location of E134 near the actual position of the lipid/water interface could be a strategic element in the mechanism of activation of rhodopsin.

Photoreactions of Metarhodopsin III

Meta III is an inactive intermediate thermally formed following light activation of the visual pigment rhodopsin. It is produced from the Meta I/Meta II photoproduct equilibrium of rhodopsin by a thermal isomerization of the protonated Schiff base C=N bond of Meta I, and its chromophore configuration is therefore all-trans 15-syn. In contrast to the dark state of rhodopsin, which catalyzes exclusively the cis to trans isomerization of the C11=C12 bond of its 11-cis 15-anti chromophore, Meta III does not acquire this photoreaction specificity. Instead, it allows for light-dependent syn to anti isomerization of the C15=N bond of the protonated Schiff base, yielding Meta II, and for trans to cis isomerizations of C11=C12 and C9=C10 of the retinal polyene, as shown by FTIR spectroscopy. The 11-cis and 9-cis 15-syn isomers produced by the latter two reactions are not stable, decaying on the time scale of few seconds to dark state rhodopsin and isorhodopsin by thermal C15=N isomerization, as indicated by time-resolved FTIR methods. Flash photolysis of Meta III produces therefore Meta II, dark state rhodopsin, and isorhodopsin. Under continuous illumination, the latter two (or its unstable precursors) are converted as well to Meta II by presumably two different mechanisms.

Rhodopsin photoproducts in 2D crystals

The published electron microscope and X-ray structures of rhodopsin have made available a detailed picture of the inactive dark state of rhodopsin. Yet, the photointermediates of rhodopsin that ultimately lead to the activated receptor species still await a similar analysis. Such an analysis first requires the generation and characterization of the photoproducts that can be obtained in crystals of rhodopsin. We therefore studied with Fourier-transform infrared (FTIR) difference spectroscopy the photoproducts in 2D crystals of bovine rhodopsin in a p22(1)2(1) crystal form. The spectra obtained by cryotrapping revealed that in this crystal form the still inactive early intermediates batho, lumi, and meta I are similar to those obtained from rhodopsin in native disk membranes, although the transition from lumi to meta I is shifted to a higher temperature. However, at room temperature, the formation of the active state, meta II, is blocked in the crystalline environment. Instead, an intermediate state is formed that bears some features of meta II but lacks the specific conformational changes required for activity. Despite being unable to activate its cognate G protein, transducin, to a significant extent, this intermediate state is capable of interacting with functional transducin-derived peptides to a limited extent. Therefore, while unable to support formation of rhodopsin's active state meta II, 2D p22(1)2(1) crystals proved to be very suitable for determining 3D structures of its still inactive precursors, batho, lumi, and meta I. In future studies, FTIR spectroscopy may serve as a sensitive assay to screen crystals grown under altered conditions for potential formation of the active state, meta II.

Deactivation of rhodopsin in the transition from the signaling state meta II to meta III involves a thermal isomerization of the retinal chromophore C[double bond]D

Light-induced isomerization of rhodopsin's retinal chromophore to the activating all-trans geometry initializes the formation of the active receptor state, Meta II. In the absence of peripheral regulatory proteins, the activity of Meta II is switched off spontaneously by two independent pathways: either by hydrolysis of the retinal Schiff base and dissociation of the light receptor into apoprotein opsin plus free retinal or by formation of Meta III, an inactive species with intact retinal protonated Schiff base absorbing at 470 nm. By FTIR spectroscopy on rhodopsin reconstituted with isotopically labeled chromophores in combination with quantum mechanical DFT calculations, we show that the deactivating step during formation of Meta III involves a thermal isomerization of the chromophore C[double bond]N, such that the chromophore in Meta III is all-trans-15-syn. This isomerization step is catalyzed by the protein environment and proceeds via Meta I, as suggested by its dependence on pH and on properties of the lipid/detergent environment of the protein. In the long term, Meta III decays likewise to opsin and free retinal by slow hydrolysis of the Schiff base.

Structural changes of water molecules during the photoactivation processes in bovine rhodopsin

Internal water molecules of rhodopsins play an important role in stabilizing the crucial ion pair comprised by the protonated retinal Schiff base and its counterion. Previous low-temperature FTIR spectroscopy of archaeal rhodopsins observed water O-D stretching vibrations at 2400-2100 cm(-1) in D(2)O, corresponding to strong hydrogen bonds. Since a water molecule bridges the protonated Schiff base and an aspartate in archaeal rhodopsins, the observed water molecules presumably hydrate the negative charges in the Schiff base region. In contrast, the FTIR spectroscopy data of bovine rhodopsin presented here revealed that there are no spectral changes of water molecules under strongly hydrogen-bonding conditions (in the range <2400 cm(-1) for O-D stretch) during the photoactivation processes. The only observed water bands were located in the >2500 cm(-1) region that corresponds to weak hydrogen bonding. These results imply that the ion pair state in vertebrate visual rhodopsins is stabilized in a manner different from that in archaeal rhodopsins. In addition, the internal water molecules that hydrate the negative charges do not play important role in the photoactivation processes of rhodopsin that involve proton transfer from the Schiff base to Glu113 upon formation of Meta II. Structural changes of the H-D exchangeable peptide amide of a beta-sheet are observed upon formation of metarhodopsin II, suggesting that motion of a beta-sheet is coupled to the proton transfer reaction from the Schiff base to its counterion.

Retinal counterion switch in the photoactivation of the G protein-coupled receptor rhodopsin

The biological function of Glu-181 in the photoactivation process of rhodopsin is explored through spectroscopic studies of site-specific mutants. Preresonance Raman vibrational spectra of the unphotolyzed E181Q mutant are nearly identical to spectra of the native pigment, supporting the view that Glu-181 is uncharged (protonated) in the dark state. The pH dependence of the absorption of the metarhodopsin I (Meta I)-like photoproduct of E181Q is investigated, revealing a dramatic shift of its Schiff base pKa compared with the native pigment. This result is most consistent with the assignment of Glu-181 as the primary counterion of the retinylidene protonated Schiff base in the Meta I state, implying that there is a counterion switch from Glu-113 in the dark state to Glu-181 in Meta I. We propose a model where the counterion switch occurs by transferring a proton from Glu-181 to Glu-113 through an H-bond network formed primarily with residues on extracellular loop II (EII). The resulting reorganization of EII is then coupled to movements of helix III through a conserved disulfide bond (Cys110-Cys187); this process may be a general element of G protein-coupled receptor activation.

Structural changes in lumirhodopsin and metarhodopsin I studied by their photoreactions at 77 K

The functional process of rhodopsin is initiated by cis-trans photoisomerization of the retinal chromophore. One of the primary intermediates, bathorhodopsin (Batho), is stable at 77 K, and structural changes in Batho are limited around the chromophore. Then, relaxation of Batho leads to helix opening at the cytoplasmic surface in metarhodopsin II (Meta II), which allows activation of a G protein transducin. Two intermediates, lumirhodopsin (Lumi) and metarhodopsin I (Meta I), appear between Batho and Meta II, and can be stabilized at 200 and 240 K, respectively. A photoaffinity labeling experiment reported that formation of Lumi accompanied flip-over of the beta-ionone ring of the retinal chromophore so that the ring portion was attached to Ala169 of helix IV [Borhan, B., Souto, M. L., Imai, H., Shichida, Y., and Nakanishi, K. (2000) Science 288, 2209-2212]. According to the crystal structure of bovine rhodopsin, the distance between the labeled C3 atom of the chromophore and Ala169 was >15 A [Palczewski, K., Kumasaka, T., Hori, T., Behnke, C. A., Motoshima, H., Fox, B. A., Le Trong, I., Teller, D. C., Okada, T., Stenkamp, R. E., Yamamoto, M., and Miyano, M. (2000) Science 289, 739-745]. These facts suggest that global protein structural changes such as helix motions take place in Lumi. In the study presented here, Lumi and Meta I are illuminated at 77 K, and protein structural changes are probed by Fourier transform infrared (FTIR) spectroscopy. We found that Lumi can be photoconverted to rhodopsin at 77 K from the IR spectral analysis of the photoproducts of Lumi. In contrast, more complex spectra were obtained for the photoproducts of Meta I at 77 K, implying that the protein structure of Meta I is considerably altered so as not to be reverted to the original state at 77 K. Thus, these photoreaction experiments with Lumi and Meta I at 77 K suggested the presence of global protein structural changes in the process between them. We concluded that the helix motions do not occur at Lumi, but at Meta I, and the flip-over of the beta-ionone ring reported by the photoaffinity labeling takes place through the specific reaction channel without a change in the global structure.

Fourier transform IR spectroscopy study for new insights into molecular properties and activation mechanisms of visual pigment rhodopsin

Fourier transform IR (FTIR) spectroscopy has been successfully applied in recent years to examine the functional and structural properties of the membrane protein rhodopsin, a prototype G protein coupled receptor. Unlike UV-visible spectroscopy, FTIR spectroscopy is structurally sensitive. It may give us both global information about the conformation of the protein and very detailed information about the retinal chromophore and all other functional groups, even when these are not directly related to the chromophore. Furthermore, it can be successfully applied to the photointermediates of rhodopsin, including the active receptor species, metarhodopsin II, and its decay products, which is not expected presently or even in the near future from crystallographic approaches. In this review we show how FTIR spectroscopy has significantly contributed to the understanding of very different aspects of rhodopsin, comprising both structural properties and the mechanisms leading to receptor activation and deactivation.

Picosecond dynamics of G-protein coupled receptor activation in rhodopsin from time-resolved UV resonance Raman spectroscopy

The protein response to retinal chromophore isomerization in the visual pigment rhodopsin is studied using picosecond time-resolved UV resonance Raman spectroscopy. High signal-to-noise Raman spectra are obtained using a 1 kHz Ti:Sapphire laser apparatus that provides <3 ps visible (466 nm) pump and UV (233 nm) probe pulses. When there is no time delay between the pump and probe events, tryptophan modes W18, W16, and W3 exhibit decreased Raman scattering intensity. At longer pump-probe time delays of +5 and +20 ps, both tryptophan (W18, W16, W3, and W1) and tyrosine (Y1 + 2xY16a, Y7a, Y8a) peak intensities drop by up to 3%. These intensity changes are attributed to decreased hydrophobicity in the microenvironment near at least one tryptophan and one tyrosine residue that likely arise from weakened interaction with the beta-ionone ring of the chromophore following cis-to-trans isomerization. Examination of the crystal structure suggests that W265 and Y268 are responsible for these signals. These UV Raman spectral changes are nearly identical to those observed for the rhodopsin-to-Meta I transition, implying that impulsively driven protein motion by the isomerizing chromophore during the 200 fs primary transition drives key structural changes that lead to protein activation.

Proteorhodopsin is a light-driven proton pump with variable vectoriality

Proteorhodopsin, a homologue of archaeal bacteriorhodopsin (BR), belongs to a newly identified family of retinal proteins from marine bacteria, which could play an important role in the energy balance of the biosphere. We cloned the cDNA sequence of proteorhodopsin by chemical gene synthesis, expressed the protein in Escherichia coli cells, purified and reconstituted the protein in its functional active state. The photocycle characteristics were determined by time-resolved absorption and Fourier transform infrared (FT-IR) spectroscopy. The pH-dependence of the absorption spectrum indicates that the pK(a) of the primary acceptor of the Schiff base proton (Asp97) is 7.68. Generally, the photocycle of proteorhodopsin is similar to that of BR, although an L-like photocycle intermediate was not detectable. Whereas at pH>7 an M-like intermediate is formed upon illumination, at pH 5 no M-like intermediate could be detected. As the photocycle kinetics do not change between the acidic and alkaline state of proteorhodopsin, the only difference between these two forms is the protonation status of Asp97. This is corroborated by time-resolved FT-IR spectroscopy, which demonstrates that proton transfer from the retinal Schiff base to Asp97 is observed at alkaline pH, but the other vibrational changes are essentially pH-independent.After reconstitution into proteoliposomes, light-induced proton currents of proteorhodopsin were measured in a compound membrane system where proteoliposomes were adsorbed to planar lipid bilayers. Our results show that proteorhodopsin is a light-driven proton pump with characteristics similar to those of BR at alkaline pH. However, at acidic pH, the direction of proton pumping is inverted. Complementary experiments were carried out on proteorhodopsin expressed heterologously in Xenopus laevis oocytes under voltage clamp conditions. The following results were obtained. (1) At alkaline pH, proteorhodopsin mediates outwardly directed proton pumping like BR. (2) The direction of proton pumping can be inverted, when Asp97 is protonated. (3) The current can be inverted by changes of the polarity of the applied voltage. (4) The light intensity-dependence of the photocurrents leads to the conclusion that the alkaline form of proteorhodopsin shows efficient proton pumping after sequential excitation by two photons.

Rhodopsin: insights from recent structural studies

The recent report of the crystal structure of rhodopsin provides insights concerning structure-activity relationships in visual pigments and related G protein-coupled receptors (GPCRs). The seven transmembrane helices of rhodopsin are interrupted or kinked at multiple sites. An extensive network of interhelical interactions stabilizes the ground state of the receptor. The ligand-binding pocket of rhodopsin is remarkably compact, and several chromophore-protein interactions were not predicted from mutagenesis or spectroscopic studies. The helix movement model of receptor activation, which likely applies to all GPCRs of the rhodopsin family, is supported by several structural elements that suggest how light-induced conformational changes in the ligand-binding pocket are transmitted to the cytoplasmic surface. The cytoplasmic domain of the receptor includes a helical domain extending from the seventh transmembrane segment parallel to the bilayer surface. The cytoplasmic surface appears to be approximately large enough to bind to the transducin heterotrimer in a one-to-one complex. The structural basis for several unique biophysical properties of rhodopsin, including its extremely low dark noise level and high quantum efficiency, can now be addressed using a combination of structural biology and various spectroscopic methods. Future high-resolution structural studies of rhodopsin and other GPCRs will form the basis to elucidate the detailed molecular mechanism of GPCR-mediated signal transduction.

Attenuated total reflection Fourier transform infrared spectroscopy of redox transitions in photosynthetic reaction centers: comparison of perfusion- and light-induced difference spectra

Chemically induced Fourier transform infrared difference spectra associated with redox transitions of several primary electron donors and acceptors in photosynthetic reaction centers (RCs) have been compared with the light-induced FTIR difference spectra involving the same cofactors. The RCs are deposited on an attenuated total reflection (ATR) prism and form a film that is enclosed in a flow cell. Redox transitions in the film of RCs can be repetitively induced either by perfusion of buffers poised at different redox potentials or by illumination. The perfusion-induced ATR-FTIR difference spectra for the oxidation of the primary electron donor P in the RCs of the purple bacteria Rb. sphaeroides and Rp. viridis and P700 in the photosystem 1 of Synechocystis 6803, as well as the Q(A)/Q(A) transition of the quinone acceptor (Q(A)) in Rb. sphaeroides RCs are reported for the first time. They are compared with the light-induced ATR-FTIR difference spectra P+Q(A)/PQ(A) for the RCs of Rb. sphaeroides and P700+/P700 for photosystem 1. It is shown that the perfusion-induced and light-induced ATR-FTIR difference spectra recorded on the same RC film display identical signal to noise ratios when they are measured under comparable conditions. The ATR-FTIR difference spectra are very similar to the equivalent FTIR difference spectra previously recorded upon photochemical or electrochemical excitation of these RCs in the more conventional transmission mode. The ATR-FTIR technique requires a smaller amount of sample compared with transmission FTIR and allows precise control of the aqueous environment of the RC films.

Time-resolved resonance Raman analysis of chromophore structural changes in the formation and decay of rhodopsin's BSI intermediate

Time-resolved resonance Raman microchip flow experiments are performed to obtain the vibrational spectrum of the chromophore in rhodopsin's BSI intermediate and to probe structural changes in the bathorhodopsin-to-BSI and BSI-to-lumirhodopsin transitions. Kinetic Raman spectra from 250 ns to 3 micros identify the key vibrational features of BSI. BSI exhibits relatively intense HOOP modes at 886 and 945 cm(-1) that are assigned to C(14)H and C(11)H=C(12)H A(u) wags, respectively. This result suggests that in the bathorhodopsin-to-BSI transition the highly strained all-trans chromophore has relaxed in the C(10)-C(11)=C(12)-C(13) region, but is still distorted near C(14). The low frequency of the 11,12 A(u) HOOP mode in BSI compared with that of lumirhodopsin and metarhodopsin I indicates weaker coupling between the 11H and 12H wags due to residual distortion of the BSI chromophore near C(11)=C(12). The C=NH(+) stretching mode in BSI at 1653 cm(-1) exhibits a normal deuteriation induced downshift of 23 cm(-1), implying that there is no significant structural rearrangement of the Schiff base counterion region in the transition of bathorhodopsin to BSI. However, a dramatic Schiff base environment change occurs in the BSI-to-lumirhodopsin transition, because the 1638 cm(-1) C=NH(+) stretching mode in lumirhodopsin is unusually low and shifts only 7 cm(-1) in D(2)O, suggesting that it has essentially no H-bonding acceptor. With these data we can for the first time compare and discuss the room temperature resonance Raman vibrational structure of all the key intermediates in visual excitation.

Conformation and stability of alpha-helical membrane proteins. 2. Influence of pH and salts on stability and unfolding of rhodopsin

We studied the stability and pH-induced denaturation of rhodopsin and its photoproducts as a model for alpha-helical membrane proteins. The increased stability of the dark state of rhodopsin as compared to its photoproduct states allows the initiation of unfolding of the protein by light-dependent isomerization of the chromophore. We could therefore characterize the transition from the native to either acid or alkaline denatured states by light-induced Fourier transform infrared difference spectroscopy, UV-visible spectroscopy, and intrinsic tryptophan fluorescence spectroscopy. The results indicate a loss of important tertiary interactions within the protein and between the protein and the retinal chromophore in the denatured state, despite that the secondary structure of the protein is almost fully retained during the transition. We therefore propose that in this denatured state the protein adopts the conformation of a loose bundle of preserved, but only weakly interacting, transmembrane helices with a largely des-oriented and partly solvent-exposed chromophore. We further characterized the influence of salts on the stability of the rhodopsin helix bundle, which was found to follow the Hofmeister series. We found that the effect of sodium chloride may be stabilizing or destabilizing, depending on the intrinsic stability of the examined protein conformation and on salt concentration. In particular, sodium chloride is shown to counteract the formation of the denatured loose bundle state presumably by increasing the lateral pressure on the helix bundle, thereby stabilizing native-like tertiary contacts within the protein.

Suramin affects coupling of rhodopsin to transducin

Suramin, a polysulfonated naphthylurea, is under investigation for the treatment of several cancers. It interferes with signal transduction through G(s), G(i), and G(o), but structural and kinetic aspects of the molecular mechanism are not well understood. Here, we have investigated the influence of suramin on coupling of bovine rhodopsin to G(t), where G-protein activation and receptor structure can be monitored by spectroscopic in vitro assays. G(t) fluorescence changes in response to rhodopsin-catalyzed nucleotide exchange reveal that suramin inhibits G(t) activation by slowing down the rate of complex formation between metarhodopsin-II and G(t). The metarhodopsin-I/-II photoproduct equilibrium, GTPase activity, and nucleotide uptake by G(t) are unaffected. Attenuated total reflection Fourier transform infrared spectroscopy shows that the structure of rhodopsin, metarhodopsin-II, and the metarhodopsin-II G(t) complex is also not altered. Instead, suramin dissociates G(t) from disk membranes in the dark, whereas metarhodopsin-II G(t) complexes are stable. Förster resonance energy transfer suggests a suramin-binding site near Trp(207) on the G(t alpha) subunit (K(d) approximately 0.5 microM). The kinetic analyses and the structural data are consistent with a specific perturbation by suramin of the membrane attachment site on G(t alpha). Disruption of membrane anchoring may contribute to some of the effects of suramin exerted on other G-proteins.

Rhodopsin: structural basis of molecular physiology

The crystal structure of rod cell visual pigment rhodopsin was recently solved at 2.8-A resolution. A critical evaluation of a decade of structure-function studies is now possible. It is also possible to begin to explain the structural basis for several unique physiological properties of the vertebrate visual system, including extremely low dark noise levels as well as high gain and color detection. The ligand-binding pocket of rhodopsin is remarkably compact, and several apparent chromophore-protein interactions were not predicted from extensive mutagenesis or spectroscopic studies. The transmembrane helices are interrupted or kinked at multiple sites. An extensive network of interhelical interactions stabilizes the ground state of the receptor. The helix movement model of receptor activation, which might apply to all G protein-coupled receptors (GPCRs) of the rhodopsin family, is supported by several structural elements that suggest how light-induced conformational changes in the ligand-binding pocket are transmitted to the cytoplasmic surface. The cytoplasmic domain of the receptor is remarkable for a carboxy-terminal helical domain extending from the seventh transmembrane segment parallel to the bilayer surface. Thus the cytoplasmic surface appears to be approximately the right size to bind to the transducin heterotrimer in a one-to-one complex. Future high-resolution structural studies of rhodopsin and other GPCRs will form a basis to elucidate the detailed molecular mechanism of GPCR-mediated signal transduction.

Signaling states of rhodopsin: absorption of light in active metarhodopsin II generates an all-trans-retinal bound inactive state

Absorption of light in rhodopsin leads through 11-cis- and all-trans-retinal isomerization, proton transfers, and structural changes to the active G-protein binding meta-II state. When meta-II is photolysed by blue light absorption, the activating pathway is apparently reverted, and rhodopsin is photoregenerated. However, the product formed, a P subspecies with A(max) = 500 nm (P(500)), is different from the ground state based on the following observations: (i) the ground state fingerprint of 11-cis-retinal does not appear in the infrared spectra, although the proton transfers and structural changes are reverted; (ii) extraction of the retinal from P(500) does not yield the expected stoichiometric amount of 11-cis-retinal but predominantly yields all-trans-retinal; (iii) the infrared spectrum of P(500) is similar to the classical meta-III intermediate, which arises from meta-II by thermal decay; and (iv) both P(500) and meta-III can be photoconverted to meta-II with the same changes in the infrared spectrum and without a significant change in the isomerization state of the extracted chromophore. The data indicate the presence of a "second switch" between active and inactive conformations that operates by photolysis but without isomerization around the C(11)-C(12) double bond. This emphasizes the exclusivity of the ground state, which is only accessible by the metabolic regeneration with 11-cis-retinal.

Chromophore structure in lumirhodopsin and metarhodopsin I by time-resolved resonance Raman microchip spectroscopy

Time-resolved resonance Raman microchip flow experiments have been performed on the lumirhodopsin (Lumi) and metarhodopsin I (Meta I) photointermediates of rhodopsin at room temperature to elucidate the structure of the chromophore in each species as well as changes in protein-chromophore interactions. Transient Raman spectra of Lumi and Meta I with delay times of 16 micros and 1 ms, respectively, are obtained by using a microprobe system to focus displaced pump and probe laser beams in a microfabricated flow channel and to detect the scattering. The fingerprint modes of both species are very similar and characteristic of an all-trans chromophore. Lumi exhibits a relatively normal hydrogen-out-of-plane (HOOP) doublet at 951/959 cm(-1), while Meta I has a single HOOP band at 957 cm(-1). These results suggest that the transitions from bathorhodopsin to Lumi and Meta I involve a relaxation of the chromophore to a more planar all-trans conformation and the elimination of the structural perturbation that uncouples the 11H and 12H wags in bathorhodopsin. Surprisingly, the protonated Schiff base C=N stretching mode in Lumi (1638 cm(-1)) is unusually low compared to those in rhodopsin and bathorhodopsin, and the C=ND stretching mode shifts down by only 7 cm(-1) in D2O buffer. This indicates that the Schiff base hydrogen bonding is dramatically weakened in the bathorhodopsin to Lumi transition. However, the C=N stretching mode in Meta I is found at 1654 cm(-1) and exhibits a normal deuteration-induced downshift of 24 cm(-1), identical to that of the all-trans protonated Schiff base. The structural relaxation of the chromophore-protein complex in the bathorhodopsin to Lumi transition thus appears to drive the Schiff base group out of its hydrogen-bonded environment near Glu113, and the hydrogen bonding recovers to a normal solvated PSB value but presumably a different hydrogen bond acceptor with the formation of Meta I.

The photobleaching sequence of a short-wavelength visual pigment

The photobleaching pathway of a short-wavelength cone opsin purified in delipidated form (lambda(max) = 425 nm) is reported. The batho intermediate of the violet cone opsin generated at 45 K has an absorption maximum at 450 nm. The batho intermediate thermally decays to the lumi intermediate (lambda(max) = 435 nm) at 200 K. The lumi intermediate decays to the meta I (lambda(max) = 420 nm) and meta II (lambda(max) = 388 nm) intermediates at 258 and 263 K, respectively. The meta II intermediate decays to free retinal and opsin at >270 K. At 45, 75, and 140 K, the photochemical excitation of the violet cone opsin at 425 nm generates the batho intermediate at high concentrations under moderate illumination. The batho intermediate spectra, generated via decomposing the photostationary state spectra at 45 and 140 K, are identical and have properties typical of batho intermediates of other visual pigments. Extended illumination of the violet cone opsin at 75 K, however, generates a red-shifted photostationary state (relative to both the dark and the batho intermediates) that has as absorption maximum at approximately 470 nm, and thermally reverts to form the normal batho intermediate when warmed to 140 K. We conclude that this red-shifted photostationary state is a metastable state, characterized by a higher-energy protein conformation that allows relaxation of the all-trans chromophore into a more planar conformation. FTIR spectroscopy of violet cone opsin indicates conclusively that the chromophore is protonated. A similar transformation of the rhodopsin binding site generates a model for the VCOP binding site that predicts roughly 75% of the observed blue shift of the violet cone pigment relative to rhodopsin. MNDO-PSDCI calculations indicate that secondary interactions involving the binding site residues are as important as the first-order chromophore protein interactions in mediating the wavelength maximum.

Distinct roles of the second and third cytoplasmic loops of bovine rhodopsin in G protein activation

In contrast to the extensive studies of light-induced conformational changes in rhodopsin, the cytoplasmic architecture of rhodopsin related to the G protein activation and the selective recognition of G protein subtype is still unclear. Here, we prepared a set of bovine rhodopsin mutants whose cytoplasmic loops were replaced by those of other ligand-binding receptors, and we compared their ability for G protein activation in order to obtain a clue to the roles of the second and third cytoplasmic loops of rhodopsin. The mutants bearing the third loop of four other G(o)-coupled receptors belonging to the rhodopsin superfamily showed significant G(o) activation, indicating that the third loop of rhodopsin possibly has a putative site(s) related to the interaction of G protein and that it is simply exchangeable with those of other G(o)-coupled receptors. The mutants bearing the second loop of other receptors, however, had little ability for G protein activation, suggesting that the second loop of rhodopsin contains a specific region essential for rhodopsin to be a G protein-activating form. Systematic chimeric and point mutational studies indicate that three amino acids (Glu(134), Val(138), and Cys(140)) in the N-terminal region of the second loop of rhodopsin are crucial for efficient G protein activation. These results suggest that the second and third cytoplasmic loops of bovine rhodopsin have distinct roles in G protein activation and subtype specificity.