Absorption studies of neutral retinal Schiff base chromophores

The neutral retinal Schiff base is connected to opsin in UV sensing pigments and in the blue-shifted meta-II signaling state of the rhodopsin photocycle. We have designed and synthesized two model systems for this neutral chromophore and have measured their gas-phase absorption spectra in the electrostatic storage ring ELISA with a photofragmentation technique. By comparison to the absorption spectrum of the protonated retinal Schiff base in vacuo, we found that the blue shift caused by deprotonation of the Schiff base is more than 200 nm. The absorption properties of the UV absorbing proteins are thus largely determined by the intrinsic properties of the chromophore. The effect of approaching a positive charge to the Schiff base was also studied, as well as the susceptibility of the protonated and unprotonated chromophores to experience spectral shifts in different solvents.     

All-trans-N-retinylidenetryptamine Schiff base in surfactant solubilized water pools in heptane—a fluorescence study

All-trns-N-retinylidenetryptamine Schiff base was incorporated into aerosol-OT (AOT, sodium bis(2-ethylhexyl)sulphosuccinate)/heptane reverse micelles. This micellar system was used as a model to study the retinal-tryptophan interactions in retinal proteins. The retinylidene Schiff base remains stable in the presence of reverse micelle-solubilized water pools. Partition coefficient and microviscosity measurements show that the Schiff base is located in the micellar interphase. The results are discussed in terms of the interaction between the retinylidene chromophore and the active site environment of rhodopsin and bacteriorhodopsin. In the present model, the quencher and emitting units are covalently attached, and are separated by two carbon spacer units. The fluorescence emission data obtained for the micelle-intercalated Schiff base chromophore are compared with the fluorescence of the native protein and intermediates in the photochemical cycle of bacteriofhodopsin. A comparison of the data obtained for tryptamine and the Schiff base with the results available for bacteriorhodopsin and bacterioopsin reveals that there is a large degree of quenching on intercalation of the retinylidene chromophore in the vicinity of the fluorophore. Evidence provided by this model suggests that energy transfer to retinal can occur from tryptophan residues located in the retinal pocket in the native protein. Thus the retinylidene unit can act as a quencher of the energy of tryptophan, the nature and extent of which may depend on the conformation and relative orientation of the protein-bound fluorophore.     

Primary events in dim light vision: a chemical and spectroscopic approach toward understanding protein/chromophore interactions in rhodopsin

The visual pigment rhodopsin (bovine) is a 40 kDa protein consisting of 348 amino acids, and is a prototypical member of the subfamily A of G protein-coupled receptors (GPCRs). This remarkably efficient light-activated protein (quantum yield = 0.67) binds the chromophore 11-cis-retinal covalently by attachment to Lys296 through a protonated Schiff base. The 11-cis geometry of the retinylidene chromophore keeps the partially active opsin protein locked in its inactive state (inverse agonist). Several retinal analogs with defined configurations and stereochemistry have been incorporated into the apoprotein to give rhodopsin analogs. These incorporation results along with the spectroscopic properties of the rhodopsin analogs clarify the mode of entry of the chromophore into the apoprotein and the biologically relevant conformation of the chromophore in the rhodopsin binding site. In addition, difference UV, CD, and photoaffinity labeling studies with a 3-diazo-4-oxo analog of 11-cis-retinal have been used to chart the movement of the retinylidene chromophore through the various intermediate stages of visual transduction.     

Recent bioorganic studies on rhodopsin and visual transduction

Rhodopsin, the pigment responsible for vision in animals, insect and fish is a typical G protein (guanyl-nucleotide binding protein) consisting of seven transmembrane alpha helices and their interconnecting extramembrane loops. In the case of bovine rhodopsin, the best studied of the visual pigments, the chromophore is 11-cis retinal attached to the terminal amino group of Lys296 through a protonated Schiff base linkage. Photoaffinity labeling with a 3-diazo-4-oxo-retinoid shows that C-3 of the ionone ring moiety is close to Trp265 in helix F (VI) in dark inactivated rhodopsin. Irradiation causes a cis to trans isomerization of the 11-cis double bond giving rise to the highly strained intermediate bathorhodopsin. This undergoes a series of thermal relaxation through lumi-, meta-I and meta-II intermediates after which the retinal chromophore is expelled from the opsin binding pocket. Photoaffinity labeling performed with 3-diazo-4-oxoretinal at -196 degrees C for batho-, -80 degrees C for lumi-, -40 degrees C for meta-I, and 0 degrees C for meta-II rhodopsin showed that in bathorhodopsin the ring is still close to Trp265. However, in lumi-, meta-I and meta-II intermediates crosslinking occurs unexpectedly at A169 in helix D (IV). This shows that large movements in the helical arrangements and a flip over of the ring moiety accompanies the transduction (or bleaching) process. These changes in retinal/opsin interactions are necessarily accompanied by movements of the extramembrane loops, which in turn lead to activation of the G protein residing in the cytoplasmic side. Of the numerous G protein coupled receptors, this is the first time that the outline of transduction pathway has been clarified.     

Rhodopsin regeneration is accelerated via noncovalent 11-cis retinal-opsin complex--a role of retinal binding pocket of opsin

The regeneration of bovine rhodopsin from its apoprotein opsin and the prosthetic group 11-cis retinal involves the formation of a retinylidene Schiff base with the epsilon-amino group of the active lysine residue of opsin. The pH dependence of a Schiff base formation in solution follows a typical bell-shaped profile because of the pH dependence of the formation and the following dehydration of a 1-aminoethanol intermediate. Unexpectedly, however, we find that the formation of rhodopsin from 11-cis retinal and opsin does not depend on pH over a wide pH range. These results are interpreted by the Matsumoto and Yoshizawa (Nature 258 [1975] 523) model of rhodopsin regeneration in which the 11-cis retinal chromophore binds first to opsin through the beta-ionone ring, followed by the slow formation of the retinylidene Schiff base in a restricted space. We find the second-order rate constant of the rhodopsin formation is 6100+/-300 mol(-1) s(-1) at 25 degrees C over the pH range 5-10. The second-order rate constant is much greater than that of a model Schiff base in solution by a factor of more than 10(7). A previous report by Pajares and Rando (J Biol Chem 264 [1989] 6804) suggests that the lysyl epsilon-NH(2) group of opsin is protonated when the beta-ionone ring binding site is unoccupied. The acceleration of the Schiff base formation in rhodopsin is explained by stabilization of the deprotonated form of the lysyl epsilon-NH(2) group which might be induced when the beta-ionone ring binding site is occupied through the noncovalent binding of 11-cis retinal to opsin at the initial stage of rhodopsin regeneration, followed by the proximity and orientation effect rendered by the formation of noncovalent 11-cis retinal-opsin complex.     

Modulating rhodopsin receptor activation by altering the pKa of the retinal Schiff base

The visual pigment rhodopsin is a seven-transmembrane (7-TM) G protein-coupled receptor (GPCR). Activation of rhodopsin involves two pH-dependent steps: proton uptake at a conserved cytoplasmic motif between TM helices 3 and 6, and disruption of a salt bridge between a protonated Schiff base (PSB) and its carboxylate counterion in the transmembrane core of the receptor. Formation of an artificial pigment with a retinal chromophore fluorinated at C14 decreases the intrinsic pKa of the PSB and thereby destabilizes this salt bridge. Using Fourier transform infrared difference and UV-visible spectroscopy, we characterized the pH-dependent equilibrium between the active photoproduct Meta II and its inactive precursor, Meta I, in the 14-fluoro (14-F) analogue pigment. The 14-F chromophore decreases the enthalpy change of the Meta I-to-Meta II transition and shifts the Meta I/Meta II equilibrium toward Meta II. Combining C14 fluorination with deletion of the retinal beta-ionone ring to form a 14-F acyclic artificial pigment uncouples disruption of the Schiff base salt bridge from transition to Meta II and in particular from the cytoplasmic proton uptake reaction, as confirmed by combining the 14-F acyclic chromophore with the E134Q mutant. The 14-F acyclic analogue formed a stable Meta I state with a deprotonated Schiff base and an at least partially protonated protein counterion. The combination of retinal modification and site-directed mutagenesis reveals that disruption of the protonated Schiff base salt bridge is the most important step thermodynamically in the transition from Meta I to Meta II. This finding is particularly important since deprotonation of the retinal PSB is known to precede the transition to the active state in rhodopsin activation and is consistent with models of agonist-dependent activation of other GPCRs.     

MAGIC ANGLE SPINNING NMR STUDIES ON THE METARHODOPSIN II INTERMEDIATE OF BOVINE RHODOPSIN: EVIDENCE FOR AN UNPROTONATED SCHIFF BASE

Magic angle spinning (MAS)13C-NMR spectra of the metarhodopsin II intermediate have been obtained using bovine rhodopsin regenerated with retinal 13C-labeled at the C-13 and C-15 positions to investigate the protonation state of the retinal Schiff base linkage. The 13C-labeled rhodopsin was reconstituted into 1,2-dipalmitoleoylphosphatidylcholine bilayers to increase the amount of meta II trapped at low temperature. Both the 13C-15 (159.2 ppm) and 13C-13 (144.0 ppm) isotropic chemical shifts are characteristic of an unprotonated Schiff base, while the 13C-15 shift is significantly different from that of retinal (191 ppm) or a tetrahedral carbinolamine group (70-90 ppm) previously proposed as an intermediate in the hydrolysis of the Schiff base at the meta II stage. This rules out the possibility that meta II non-covalently binds retinal or is a carbinolamine intermediate and provides convincing evidence that Schiff base deprotonation occurs in the meta I-meta II transition, an event that is likely to be important in triggering the activation of transducin.     

LIGHT-INDUCED PERTURBATION OF AROMATIC RESIDUES IN BOVINE RHODOPSIN AND BACTERIORHODOPSIN*

Light-induced changes in the UV absorption spectrum of bovine rod outer segment membranes were measured by conventional difference spectroscopy and by flash photolysis methods. Different thermal intermediates of rhodopsin (lumirhodopsin, metarhodopsin I, metarhodopsin II, and meta-rhodopsin III) have absorption spectra in the ultraviolet which differ from the rhodopsin spectrum and from each other. The spectra associated with metarhodopsin I, metarhodopsin II, and metarhodopsin III are characteristic of perturbation of a small number of tyr. and/or trp residues, most likely one trp residue. These aromatic residues are in the neighborhood of the retinal Schiff base and undergo coordinated changes of interaction with retinal during the bleaching sequence. At the metarhodopsin II stage, the magnitude of the UV spectral changes is consistent with the exposure of a previously shielded trp residue to an aqueous environment. The present results are consistent with previous spectral studies which limit the extent of light-induced conformational changes to regions of the protein in the neighborhood of the retinal Schiff base. An analogous study was made on light-adapted purple membranes of Halobacterium halobium. The UV absorption spectrum associated with the deprotonated Schiff base intermediate of the trans-bacteriorhodopsin cycle is indicative, in part, of aromatic residue perturbation. However, significant changes in the secondary and tertiary structures of the bacterio-rhodopsin protein characteristic of a delocalized conformational change are unlikely at this intermediate stage.     

Engineering a rhodopsin protein mimic

Due to the difficulties in handling and manipulating membrane-bound proteins, such as rhodopsin, and the lack of crystallographic information on the cone opsins, we have opted to engineer a protein mimic of the transmembrane G-protein coupled receptor. Human cellular retinoic acid binding protein (CRABPII), a well studied and characterized protein, has been reengineered into a protein that now will bind retinal as a protonated Schiff base with high binding affinity (Kd = 2 nM) mimicking that of rhodopsin.     

Functional and Photochemical Characterization of a Light‐Driven Proton Pump from the Gammaproteobacterium Pantoea vagans

Photoactive retinal proteins are widely distributed throughout the domains of the microbial world (i.e., bacteria, archaea, and eukarya). Here we describe three retinal proteins belonging to a phylogenetic clade with a unique DTG motif. Light‐induced decrease in the environmental pH and its inhibition by carbonyl cyanide m‐chlorophenylhydrazone revealed that these retinal proteins function as light‐driven outward electrogenic proton pumps. We further characterized one of these proteins, Pantoea vagans rhodopsin (PvR), spectroscopically. Visible spectroscopy and high‐performance liquid chromatography revealed that PvR has an absorption maximum at 538 nm with the retinal chromophore predominantly in the all‐trans form (>90%) under both dark and light conditions. We estimated the pK_a values of the protonated Schiff base of the retinal chromophore and its counterion as approximately 13.5 and 2.1, respectively, by using pH titration experiments, and the photochemical reaction cycle of PvR was measured by time‐resolved flash‐photolysis in the millisecond timeframe. We observed a blue‐shifted and a red‐shifted intermediate, which we assigned as M‐like and O‐like intermediates, respectively. Decay of the M‐like intermediate was highly sensitive to environmental pH, suggesting that proton uptake is coupled to decay of the M‐like intermediate. From these results, we propose a putative model for the photoreaction of PvR.     

Rhodopsin deactivation is affected by mutations of Tyrl91

The 9-methyl group of 11-cis retinal is important in the efficient formation of the active conformation of rhodopsin, Meta II. Here, Tyrl91 rhodopsin mutants were generated because of its proximity to that methyl group in the dark structure. If photoactivation results in movement of the 9-methyl group toward Tyrl91, the steric interactions involved with activation and/or deactivation might not be as tightly coupled in mutant proteins with smaller amino acids at that position. Tyrl91 mutations have no effect on the dark pigment. However, after photobleaching, the lifetime of Meta II is shorter; Meta II decays quickly into two inactive species: (1) a Meta III or Meta III-like species and (2) opsin and free retinal. The Meta III-like fraction maintains the covalent Schiff base linkage of the chromophore much longer than the wild type. On the other hand, the fast chromophore release is similar to cone pigments. Taken together, the data suggest that the role of the 9-methyl group after photo-isomerization is not only to form Meta II efficiently, but also to maintain its active conformation and allow for the timely hydrolysis of the Schiff base. Perturbation of this interaction effects changes in the hydrolysis of the Schiff base and for the case of the Y191A mutation the folded structure of the protein after photobleaching.     

Coupling of protonation switches during rhodopsin activation

Recent studies of the activation mechanism of rhodopsin involving Fourier-transform infrared spectroscopy and a combination of chromophore modifications and site-directed mutagenesis reveal an allosteric coupling between two protonation switches. In particular, the ring and the 9-methyl group of the all-trans retinal chromophore serve to couple two proton-dependent activation steps: proton uptake by a cytoplasmic network between transmembrane (TM) helices 3 and 6 around the conserved ERY (Glu-Arg-Tyr) motif and disruption of a salt bridge between the retinal protonated Schiff base (PSB) and a protein counterion in the TM core of the receptor. Retinal analogs lacking the ring or 9-methyl group are only partial agonists--the conformational equilibrium between inactive Meta I and active Meta II photoproduct states is shifted to Meta I. An artificial pigment was engineered, in which the ring of retinal was removed and the PSB salt bridge was weakened by fluorination of C14 of the retinal polyene. These modifications abolished allosteric coupling of the proton switches and resulted in a stabilized Meta I state with a deprotonated Schiff base (Meta I(SB)). This state had a partial Meta II-like conformation due to disruption of the PSB salt bridge, but still lacked the cytoplasmic proton uptake reaction characteristic of the final transition to Meta II. As activation of native rhodopsin is known to involve deprotonation of the retinal Schiff base prior to formation of Meta II, this Meta I(SB) state may serve as a model for the structural characterization of a key transient species in the activation pathway of a prototypical G protein-coupled receptor.     

Retinal counterion switch mechanism in vision evaluated by molecular simulations

Photoisomerization of the retinylidene chromophore of rhodopsin is the starting point in the vision cascade. A counterion switch mechanism that stabilizes the retinal protonated Schiff base (PSB) has been proposed to be an essential step in rhodopsin activation. On the basis of vibrational and UV-visible spectroscopy, two counterion switch models have emerged. In the first model, the PSB is stabilized by Glu181 in the meta I state, while in the most recent proposal, it is stabilized by Glu113 as well as Glu181. We assess these models by conducting a pair of microsecond scale, all-atom molecular dynamics simulations of rhodopsin embedded in a 99-lipid bilayer of SDPC, SDPE, and cholesterol (2:2:1 ratio) varying the starting protonation state of Glu181. Theoretical simulations gave different orientations of retinal for the two counterion switch mechanisms, which were used to simulate experimental 2H NMR spectra for the C5, C9, and C13 methyl groups. Comparison of the simulated 2H NMR spectra with experimental data supports the complex-counterion mechanism. Hence, our results indicate that Glu113 and Glu181 stabilize the retinal PSB in the meta I state prior to activation of rhodopsin.     

THE ORIGIN OF THE RED-SHIFTED ABSORPTION MAXIMUM OF THE M412 INTERMEDIATE IN THE BACTERIORHODOPSIN PHOTOCYCLE

The factors that red shift the absorption maximum of the retinal Schiff base chromophore in the M₄₁₂ intermediate of bacteriorhodopsin photocycle relative to absorption in solution were investigated using a series of artificial pigments and studies of model compounds in solution. The artificial pigments derived from retinal analogs that perturb chromophore-protein interactions in the vicinity of the ring moiety indicate that a considerable part of the red shift may originate from interactions in the vicinity of the Schiff base linkage. Studies with model compounds revealed that hydrogen bonding to the Schiff base moiety can significantly red shift the absorption maximum. Furthermore, it was demonstrated that although s-trans ring-chain planarity prevails in the M₄₁₂ intermediate it does not contribute significantly (only ca 750 cm⁻¹) to the opsin shift observed in M₄₁₂. It is suggested that in M₄₁₂, the Schiff base linkage is hydrogen bonded to bound water and/or protein residues inducing a considerable red shift in the absorption maximum of the retinal chromophore.     

PHOTOCHEMISTRY OF METHYLATED RHODOPSINS

Abstract— Rhodopsin, in which the active-site Schiff-base lysine has been chemically modified by monomethylation, is unable to form the deprotonated Schiff base bleaching intermediate, rnetarhodop-sin II. The photochemistry of the methylated Schiff base rhodopsin stops at the metarhodopsin I stage, which then slowly decays to all-trans retinal and opsin. Methylation of the non active-site lysines does not block the photochemical transformation but does speed up the formation and decay of the metarhodopsins.     

Constraints of opsin structure on the ligand-binding site: studies with ring-fused retinals

Ring-fused retinal analogs were designed to examine the hula-twist mode of the photoisomerization of the 9-cis retinylidene chromophore. Two 9-cis retinal analogs, the C11-C13 five-membered ring-fused and the C12-C14 five-membered ring-fused retinal derivatives, formed the pigments with opsin. The C11-C13 ring-fused analog was isomerized to a relaxed all-trans chromophore (lambda(max) > 400 nm) at even -269 degrees C and the Schiff base was kept protonated at 0 degrees C. The C12-C14 ring-fused analog was converted photochemically to a bathorhodopsin-like chromophore (lambda(max) = 583 nm) at -196 degrees C, which was further converted to the deprotonated Schiff base at 0 degrees C. The model-building study suggested that the analogs do not form pigments in the retinal-binding site of rhodopsin but form pigments with opsin structures, which have larger binding space generated by the movement of transmembrane helices. The molecular dynamics simulation of the isomerization of the analog chromophores provided a twisted C11-C12 double bond for the C12-C14 ring-fused analog and all relaxed double bonds with a highly twisted C10-C11 bond for the C11-C13 ring-fused analog. The structural model of the C11-C13 ring-fused analog chromophore showed a characteristic flip of the cyclohexenyl moiety toward transmembrane segments 3 and 4. The structural models suggested that hula twist is a primary process for the photoisomerization of the analog chromophores.     

LOW-TEMPERATURE TRAPPING OF EARLY PHOTOINTERMEDIATES OF α-ISORHODOPSIN

Abstract— a-Isorhodopsin, an artificial visual pigment with a 9- cis -4,5-dehydro-5,6-dihydro(a)retinal chromophore, was photolyzed at low temperatures and absorption difference spectra were collected as the sample was warmed. A bathorhodopsin (Batho)-like intermediate absorbing at ca 495 nm was detected below 55 K, a blue-shifted intermediate (BSI)-like intermediate absorbing at ca 453 nm was observed when the temperature was raised to 60 K and a lumirhodopsin (Lumi)-like intermediate absorbing at ca 470 nm was found when the sample was warmed to 115 K. Photointermediates from this pigment were compared to those of native rhodopsin and 5,6-dihydroisorhodopsin. As in native rho-dopsin, Batho is the first intermediate detected in a-isorhodopsin, though unlike native rhodopsin at low temperatures BSI is observed prior to Lumi formation. a-Isorhodopsin behaves similarly to 5,6-dihydroisorhodopsin, with the same early intermediates observed in both artificial visual pigments lacking the C₅-C₆ double bond. The transition temperature for BSI formation is higher in a-isorhodopsin, suggesting an interaction involving the chromophore ring in BSI formation. The transition temperature for Lumi formation is similar for these two pigments as well as for native rhodopsin, suggesting comparable changes in the protein environment in that transition.     

Interaction of chromophore, 11-<Emphasis Type="Italic">cis</Emphasis>-retinal,with amino acid residues of the visual pigment rhodopsin in the region of protonated Schiff base: A molecular dynamics study

A molecular dynamics study of the dark adapted visual pigment rhodopsin molecule was carried out. The interaction of the chromophore group, 11-cis-retinal, with the nearest amino acid residues in the chromophore center of the molecule, namely, in the region of the protonated Schiff base linkage, was analyzed. Most likely, the interaction of the CH=NH bond with the negatively charged amino acid residue Glu113 cannot be described as a simple electrostatic interaction of two oppositely charged groups. One can propose that not only Glu113 but also Glu181 and Ser186 are involved in stabilization of the protonated Schiff base linkage. Accord-ing to calculations, Glu181 interacts, as the counter-ion, with the Schiff base indirectly via Ser186. The intramolecular mechanisms of protonated Schiff base stabilization in rhodopsin are discussed. Published in Russian in Izvestiya Akademii Nauk. Seriya Khimicheskaya, No. 1, pp. 19–27, January, 2007.     

Engineered Functional Recovery of Microbial Rhodopsin Without Retinal‐Binding Lysine

Definition of rhodopsin is the retinal‐binding membrane protein with the Schiff base linkage at a lysine on the 7^th transmembrane helix. However, ~ 600 microbial rhodopsins lack retinal‐binding lysine at the corresponding position (Rh‐noK) among ~ 5500 known microbial rhodopsins, suggesting that Rh‐noK has each functional role without chromophore. Here, we report successful functional recovery of Rh‐noK. Two Rh‐noKs from bacteria were heterologously expressed in Escherichia coli, which exhibited no color. When retinal‐binding lysine was introduced, one of them gained visible color. Additional mutation of the Schiff base counterion further gained proton‐pumping activity. Successful engineered functional recovery such as visible color and proton‐pump activity suggests that the Rh‐noK protein forms a characteristic structure of microbial rhodopsins.     

Inherent chirality dominates the visible/near-ultraviolet CD spectrum of rhodopsin

The visible (alpha) and near-UV (beta) CD bands of rhodopsin have been studied extensively, but their source(s) have never been definitively established. Do they result from the intrinsic chirality of the polyene chromophore of the protonated Schiff base of retinal (retPSB) or from the coupling of the transitions of this chromophore with those of protein groups? We have calculated the contributions of these two mechanisms to the CD of rhodopsin. The intrinsic CD of the retPSB chromophore was calculated using time-dependent density functional theory (TDDFT) and, for comparison, the semiempirical ZINDO method. First-order perturbation theory was used to calculate the effects of coupling of the retPSB transitions with the pi pi* transitions of the aromatic chromophores and the pi pi* and n pi* transitions of the peptide groups in rhodopsin. Calculations were performed for eight structures based upon the two molecules in the asymmetric unit of four crystal structures. The most reliable results were obtained from TDDFT calculations on the structure of Okada et al. (J. Mol. Biol. 2004, 342, 571), PDB 1U19. Averaging over the two molecules in the asymmetric unit, the intrinsic rotational strengths are 0.62 +/- 0.00 DBM (Debye-Bohr magneton) and 0.90 +/- 0.03 DBM for the alpha- and beta-bands, respectively. The contributions from coupling with protein groups are, respectively, -0.32 +/- 0.05 and -0.01 +/- 0.03 DBM. Our results show that the visible/near-UV CD bands of rhodopsin are determined by the intrinsic chirality of the retPSB chromophore and that the contributions of coupling with the protein are significantly smaller for the alpha-band and negligible for the beta-band.