Ring oxidized retinals form unusual bacteriorhodopsin analogue pigments.

Three ring oxidized retinal analogues have been isolated from the exhaustive oxidation of all-trans retinal. All-trans 4-oxoretinal and 2,3-dehydro-4-oxoretinal have similar absorption maxima to that of all-trans retinal and have been shown to be in the 6-s-cis conformation in solution. Pigments formed with bacterioopsin exhibit absorption maxima (520 nm) blue-shifted from that of bacteriorhodopsin (bR), indicating a disturbance of the external point charge by the electronegative carbonyl moiety at the 4 position. The third analogue contains a ring contracted to a cyclopentenyl-alpha,beta-dione. Unlike the majority of retinals, this analogue displays a 6-s-trans conformation in solution and has a red-shifted absorption maximum at 435 nm. The resulting bR analogue pigment (515 nm) is formed five times faster than the other oxoretinal pigments. All three oxoretinal pigments show an irreversible 20 nm blue shift upon exposure to white light. The 4-oxo and 2,3-dehydro-4-oxoretinal pigments, after irradiation, undergo a small reversible blue shift (4-8 nm) on dark adaptation. These two pigments pump protons, although with slowed photocycle kinetics, demonstrating that these structural changes (addition of the carbonyl at the C-4 and insertion of a double bond in the ring) do not block the function of the pigment. Extraction of the C-15 tritiated analogue retinals from illuminated and non-illuminated pigments of all three oxoretinals yield identical results. Therefore, any crosslinking of these oxoretinals to the protein is by linkages which are unstable to the extraction procedures.     

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.     

Combined QM/MM study of the opsin shift in bacteriorhodopsin

Combined quantum mechanical and molecular mechanical (QM/MM) calculations and molecular dynamics simulations of bacteriorhodopsin (bR) in the membrane matrix have been carried out to determine the factors that make significant contributions to the opsin shift. We found that both solvation and interactions with the protein significantly shifts the absorption maximum of the retinal protonated Schiff base, but the effects are much more pronounced in polar solvents such as methanol, acetonitrile, and water than in the protein environment. The differential solvatochromic shifts of PSB in methanol and in bR leads to a bathochromic shift of about 1800 cm(-1). Because the combined QM/MM configuration interaction calculation is essentially a point charge model, this contribution is attributed to the extended point-charge model of Honig and Nakanishi. The incorporation of retinal in bR is accompanied by a change in retinal conformation from the 6-s-cis form in solution to the 6-s-trans configuration in bR. The extension of the pi-conjugated system further increases the red-shift by 2400 cm(-1). The remaining factors are due to the change in dispersion interactions. Using an estimate of about 1000 cm(-1) in the dispersion contribution by Houjou et al., we obtained a theoretical opsin shift of 5200 cm(-1) in bR, which is in excellent agreement with the experimental value of 5100 cm(-1). Structural analysis of the PSB binding site revealed the specific interactions that make contributions to the observed opsin shift. The combined QM/MM method used in the present study provides an opportunity to accurately model the photoisomerization and proton transfer reactions in bR.     

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.     

RESONANCE RAMAN STUDIES OF BACTERIORHODOPSIN ANALOGUES

Abstract— We present the results of resonance Raman measurements on a series of bacteriorhodopsin (bR) analogues formed from synthetic retinals which have replaced the native chromophore in the active site. Specifically, 5,6-dihydro-bR, 13-desmethyl-bR, 10-methyl-bR, 14-methyl-bR, and 10.14-dimethyl-bR have been studied. All five analogues bind and form Schiff base retinal-apoprotein linkages. While the Schiff base linkages of 5,6-dihydro-bR, 13-desmethyl-bR, and 10-methyl-bR are protonated, like the native chromophore, the 14-methyl-bR, and 10,14-dimethyl-bR Schiff bases are unprotonated. These results suggest that the binding site of bacteriorhodopsin near the Schiff base moiety is different from that of rhodopsin. The protonated Schiff base -C=NH- stretching frequency of 5.6-dihydro-bR lies at 1660 cm^-1 which is unusually high for a bacteriorhodopsin based pigment. The downward shift upon deuteration is 16 cm^-1, essentially identical to that measured for bacteriorhodopsin. This and the other analogue results strongly reinforce our previous arguments that the Schiff base stretching frequency is determined in large part by two factors, the C=N force constant and the stretch interaction with C=N-H bend. On the other hand, the deuterium isotope effect is determined primarily by the stretch-bend interaction.     

Accurate evaluation of the absorption maxima of retinal proteins based on a hybrid QM/MM method

Here we improved our hybrid QM/MM methodology (Houjou et al. J Phys Chem B 2001, 105, 867) for evaluating the absorption maxima of photoreceptor proteins. The renewed method was applied to evaluation of the absorption maxima of several retinal proteins and photoactive yellow protein. The calculated absorption maxima were in good agreement with the corresponding experimental data with a computational error of <10 nm. In addition, our calculations reproduced the experimental gas-phase absorption maxima of model chromophores (protonated all-trans retinal Schiff base and deprotonated thiophenyl-p-coumarate) with the same accuracy. It is expected that our methodology allows for definitive interpretation of the spectral tuning mechanism of retinal proteins.     

ANALYZING THE RED-SHIFT CHARACTERISTICS OF AZULENIC,NAPHTHYL, OTHER RING-FUSED AND RETINYL PIGMENT ANALOGS OF BACTERIORHODOPSIN*

Prompted by the near infrared-absorbing properties of some of the azulenic bacteriorhodopsin (bR) analogs, we have analyzed their absorption characteristics along with 11 new related ring-fused analogs and the corresponding Schiff bases (SB) and protonated Schiff bases (PSB). The following three factors are believed to contribute to the total red shift of each of the pigment analogs (α_RS): perturbation of the basic chromophore (SB shift, ΔSB), protonation of the SB (PSB shift, PSBS) and protein perturbation (the opsin shift, OS). For each factor, effects of structural modifications were examined. For the red-shifted pigments, percent OS has been suggested as an alternate way of measuring protein perturbation. Computer-simulated chromophores provided evidence against any explanation involving altered shapes of the binding pocket as a major cause for absorption differences. Implications of the current bR results on preparation of further red-shifted bR and possible application to visual pigment analogs are discussed.     

Spectral tuning of shortwave-sensitive visual pigments in vertebrates

Of the four classes of vertebrate cone visual pigments, the shortwave-sensitive SWS1 class shows some of the largest shifts in lambda(max), with values ranging in different species from 390-435 nm in the violet region of the spectrum to < 360 nm in the ultraviolet. Phylogenetic evidence indicates that the ancestral pigment most probably had a lambda(max) in the UV and that shifts between violet and UV have occurred many times during evolution. In violet-sensitive (VS) pigments, the Schiff base is protonated whereas in UV-sensitive (UVS) pigments, it is almost certainly unprotonated. The generation of VS pigments in amphibia, birds and mammals from ancestral UVS pigments must involve therefore the stabilization of protonation. Similarly, stabilization must be lost in the evolution of avian UVS pigments from a VS ancestral pigment. The key residues in the opsin protein for these shifts are at sites 86 and 90, both adjacent to the Schiff base and the counterion at Glu113. In this review, the various molecular mechanisms for the UV and violet shifts in the different vertebrate groups are presented and the changes in the opsin protein that are responsible for the spectral shifts are discussed in the context of the structural model of bovine rhodopsin.     

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.     

SPECTROSCOPY OF POLYENES–III. ABSORPTION AND EMISSION SPECTRAL INVESTIGATION OF POLYENE SCHIFF BASES AND PROTONATED SCHIFF BASES RELATED TO VISUAL PIGMENTS

Abstract— A number of n -butylamine Schiff bases of polyenals related to retinals as homologues and analogues, and their protonated forms, have been studied for absorption and emission spectral properties. The polyene Schiff bases exhibit the same general features in their absorption spectra as those of the parallel polyenals except that the ^lB_u←¹A_g and π*← n singlet transitions are at substantially higher energy in the Schiff bases (the shift being larger for the π *← n transition). The Schiff bases with short polyene chainlength ( n = 2, 3 where n is the number of double bonds including C=N) do not fluoresce or phosphoresce in 3-methylpentane in the temperature range 298–77 K. The Schiff bases with intermediate chainlength ( n = 4, 5) show fluorescence at 77 K with intensity strongly dependent on the nature of solvent. The Schiff bases with relatively long chainlength ( n = 5–7) show strong or moderately strong fluorescence at 77 K and very weak fluorescence at 298 K ( n = 7) with intrinsic radiative lifetimes much longer than those estimated from the oscillator strength of the low-energy, strong absorption band (¹B_u←¹ A_g ). A discussion on the possible state order and nature of the fluorescing state of the various polyene Schiff base systems is presented.     

Exploring the molecular mechanism for color distinction in humans

We examine here the role of the red, green, and blue human opsin structures in modulating the absorption properties of 11-cis-retinal bonded to the protein via a protonated Schiff base (PSB). We built the three-dimensional structures of the human red, green, and blue opsins using homology modeling techniques with the crystal structure of bovine rhodopsin as the template. We then used quantum mechanics (QM) combined with molecular mechanics (MM) (denoted as QM/MM) techniques in conjunction with molecular dynamics to determine how the room temperature molecular structures of the three human color opsin proteins modulate the absorption frequency of the same bound 11-cis-retinal chromophore to account for the differences in the observed absorption spectra. We find that the conformational twisting of the 11-cis-retinal PSB plays an important role in the green to blue opsin shift, whereas the dipolar side chains in the binding pocket play a surprising role of red-shifting the blue opsin with respect to the green opsin, as a fine adjustment to the opsin shift. The dipolar side chains play a large role in the opsin shift from red to green.     

Photochemistry of a retinal protonated schiff-base analogue mimicking the opsin shift of bacteriorhodopsin

A retinal Schiff base analogue which artificially mimics the protein-induced red shifting of absorption in bacteriorhodopsin (BR) has been investigated with femtosecond multichannel pump probe spectroscopy. The objective is to determine if the catalysis of retinal internal conversion in the native protein BR, which absorbs at 570 nm, is directly correlated with the protein-induced Stokes shifting of this absorption band otherwise known as the "opsin shift". Results demonstrate that the red shift afforded in the model system does not hasten internal conversion relative to that taking place in a free retinal-protonated Schiff base (RPSB) in methanol solution, and stimulated emission takes place with biexponential kinetics and characteristic timescales of approximately 2 and 10.5 ps. This shows that interactions between the prosthetic group and the protein that lead to the opsin shift in BR are not directly involved in reducing the excited-state lifetime by nearly an order of magnitude. A sub-picosecond phase of spectral evolution, analogues of which are detected in photoexcited retinal proteins and RPSBs in solution, is observed after excitation anywhere within the intense visible absorption band. It consists of a large and discontinuous spectral shift in excited-state absorption and is assigned to electronic relaxation between excited states, a scenario which might also be relevant to those systems as well. Finally, a transient excess bleach component that tunes with the excitation wavelength is detected in the data and tentatively assigned to inhomogeneous broadening in the ground state absorption band. Possible sources of such inhomogeneity and its relevance to native RPSB photochemistry are discussed.     

Electric-Field Effects in 13-Demethyl-11,14-Epoxyretinal-Bacteriorhodopsin Films

Abstract— We report the results of experiments on the application of electric fields across thin, dry Alms of a bacteriorho-dopsin (BR) analog pigment in which the retinal chro-mophore has been replaced with 13-demethyl-11,14-epoxyretinal. As previously observed in other BR variants with low Schiff-base pK values, this pigment exhibits protonation and deprotonation of the Schiff base under an applied electric field, depending on the initial Schiff-base protonation state or effective pH. At low effective pH, a fast (<200 μs) deprotonation reaction dominates. At high pH, an apparently different mechanism leads to Schiff-base protonation on the time scale of seconds. Comparison of our results with a simple model suggests that the external field causes a shift in the pK of the Schiff base by1–2 pH units.     

Seven new hindered isomeric rhodopsins: A reexamination of the stereospecificity of the binding site of bovine opsin

Results of interaction of seven new geometric isomers of retinal (7-cis, 7,9-dicis; 7,11-dicis, 7,13-dicis; 9,11-dicis 7,9,11-tricis 7,9,13-tricis) with bovine opsin are reported. All of them form pigments with absorption maxima varying between 450 and 480 nm. The rates of pigment formation were generally considerably lower than those of 11-cis-retinal and the yields were less than quantitative. Implications of these results for the stereospecificity of the binding site of opsin are discussed.     

Alpha-retinals as rhodopsin chromophores--preference for the 9-Z configuration and partial agonist activity

The visual pigment rhodopsin, the photosensory element of the rod photoreceptor cell in the vertebrate retina, shows in combination with an endogenous ligand, 11-Z retinal, an astonishing photochemical performance. It exhibits an unprecedented quantum yield (0.67) in a highly defined and ultrafast photoisomerization process. This triggers the conformational changes leading to the active state Meta(rhodopsin) II. Retinal is covalently bound to Lys-296 of the protein opsin in a protonated Schiff base. The resulting positive charge delocalization over the terminal part of the polyene chain of retinal creates a conjugation defect that upon photoexcitation moves to the opposite end of the polyene. Shortening the polyene as in 4,5-dehydro,5,6-dihydro (alpha), 5,6-dihydro or 7,8-dihydro-analogs might facilitate photoisomerization of a 9-Z and a 11-Z bond. Here we describe pigment analogs generated with bovine opsin and 11-Z or 9-Z 4,5-dehydro,5,6-dihydro-retinal that were further characterized by UV-Vis and FTIR spectroscopy. The preference of opsin for native 11-Z retinal over the 9-Z isomer is reversed in 4,5-dehydro,5,6-dihydro-retinal. 9-Z 4,5-dehydro,5,6-dihydro-retinal readily generated a photosensitive pigment. This modification has no effect on the quantum yield, but affects the Batho<-->blueshifted intermediate (BSI) equilibrium and leads to a strong decrease in the G-protein activation rate because of a downshift of the pK(a) of the Meta I<-->Meta II equilibrium.     

PEPTIDE MODELS FOR THE BACTERIORHODOPSIN CHROMOPHORE. RETINYLIDENE-LYSINE SYSTEMS CONTAINING ASPARTIC ACID AND SERINE RESIDUES

Abstract— The retinylidene Schiff base derivative of seven lysine containing peptides have been prepared in order to investigate solvent and neighboring group effects, on the absorption maximum of the protonated Schiff base chromophore. The peptides studied are Boc-Aib-Lys-Aib-OMe ( 1 ), Boc-Ala-Aib-Lys-OMe ( 2 ), Boc-Ala-Aib-Lys-Aib-OMe ( 3 ), Boc-Aib-Asp-Aib-Aib-Lys-Aib-OMe ( 4 ), Boc-Aib-Asp-Aib-Ala-Aib-Lys-Aib-OMe ( 5 ), Boc-Lys-Val-Gly-Phe-OMe ( 6 ) and Boc-Ser-Ala-Lys-Val-Gly-Phe-OMe ( 7 ). In all cases protonation shifts the absorption maxima to the red by 3150–8450 cm^-1. For peptides 1–3 the protonation shifts are significantly larger in nonhydrogen bonding solvents like CHCl₃ or CH₂Cl₂ as compared to hydrogen bonding solvents like CH₃OH. The presence of a proximal Asp residue in 4 and 5 results in pronounced blue shift of the absorption maximum of the protonated Schiff base in CHCl₃, relative to peptides lacking this residue. Peptides 6 and 7 represent small segments of the bacteriorhodopsin sequence in the vicinity of Lys-216. The presence of Ser reduces the magnitude of the protonation shift.     

BATHOCHROMICITY OF RETINAL SCHIFF BASES IN CELLULOSE MATRIX

Abstract Schiff bases of all-trans-retinal (formed with n-butylamine, tryptamine and β-naphthylamine) and of benzaldehyde, trans -cinnamaldehyde and all- trans -retinal with aniline exhibit an appreciable red shift in their UV-visible maxima on intercalation in cellulose matrix relative to their absorption in solution in the absence of acid. Treatment of these model compounds with trichloroacetic acid in solution gives the corresponding protonated salts. The red shift due to the cellulose environment is, however, less than the red shift in acid solutions. However, an exception is all- trans-N -retinylidenetryptamine for which the red shift in cellulose is quite close to the corresponding value for the protonated salt in heptane and methanol. N -Benzalideneaniline and trans- N -cinnamalideneaniline, with shorter polyenic moieties, tend to show a greater bathochromic shift in cellulose. all-trans- N -Retinylidene- n -butylamine, all- trans-N -retinylidenetryptamine and all- trans-N -retinylidene-β-naphthylamine show a reduced bathochromic shift when intercalated in cellulose pretreated with a base such as n -butylamine. The chromophore of all- trans-N -retinylidenetryptamine is stabilized by the presence of the indole moiety. These results indicate the importance of hydrogen-bond interactions at the chromophore sites of rhodopsins. A mechanistic proposal for explaining protonation, stability and wavelength regulation in the opsin family of proteins is discussed.     

7-cis-porphyropsin from 7-cis-3-dehydroretinal and cattle opsin.

Abstract 7-cis-3-Dehydroretinol, prepared by photoisomerization of the all-trans isomer in a polar solvent, was found to combine with cattle opsin to form a visual pigment analogue with an absorption maximum at 464 nm. The pigment is only moderately stable in hydroxylamine or in Ammonyx LO. and cannot be purified by column chromatography using Ammonyx LO. 9-cis-Porphyropsin, prepared in a manner similar to that reported by Azuma et al., is stable and has been purified by passing through a hydroxylapatite column. Three fractions were collected with eluant of increasing ionic strength. All fractions exhibit similar absorption properties with Λ_max at 498 nm. These results further indicate that the binding of opsin is a flexible one.     

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.     

A NEW FACET IN RHODOPSIN PHOTOCHEMISTRY

Abstract— A structure is proposed for the prosthetic group of the visual pigments rhodopsin, prelumirhodopsin (bathorhodopsin) and lumirhodopsin. The intrinsic photochemical step in this model is tautomerization of the prosthetic group of rhodopsin to a hexaeneamine retrotautomer with an exomethylene group for prelumirhodopsin. Based on the proposed structures, molecular orbital calculations were carried out; the absorption maxima calculated snowed the same trends as the Λ_max values observed. An exact fit was not obtained because many interactions had to be neglected. Essential information of the laser Raman resonance spectrum of prelumirhodopsin can be interpreted based on the structures proposed by our model.
The model elucidates why some retinal derivates can and others cannot form visual pigments with opsin and visual pigments having vastly differing absorption maxima yet employ the same mechanism for their photoreaction.