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.     

Bathoproducts of rhodopsin, isorhodopsin I, and isorhodopsin II.

Bathorhodopsins were prepared by partially (10--15%) photoconverting bovine rhodopsin (11-cis chromophore) or isorhodopsin I (9-cis chromophore) at 77 degrees K; care was taken to avoid establishing photostationary states. The absorption spectra calculated for the bathorhodopsins derived from the two parent pigments are identical in their lambda max 'S, bandwidths, and extinction coefficients. This result provides further support for the hypothesis that bathorhodopsin is a common intermediate between an 11-cis pigment (rhodopsin) and a 9-cis one (isorhodopsin I) and thus probably has an all-trans chromophore. This in turn is strong evidence for the cis-trans isomerization model of the primary event in vision. The spectrum of the bathoproduct of isorhodopsin II (9,13-dicis chromophore) is different from the other pigments' bathoproducts.     

Early steps of the intramolecular signal transduction in rhodopsin explored by molecular dynamics simulations

We present molecular dynamics simulations of bovine rhodopsin in a membrane mimetic environment based on the recently refined X-ray structure of the pigment. The interactions between the protonated Schiff base and the protein moiety are explored both with the chromophore in the dark-adapted 11-cis and in the photoisomerized all-trans form. Comparison of simulations with Glu181 in different protonation states strongly suggests that this loop residue located close to the 11-cis bond bears a negative charge. Restrained molecular dynamics simulations also provide evidence that the protein tightly confines the absolute conformation of the retinal around the C12-C13 bond to a positive helicity. 11-cis to all-trans isomerization leads to an internally strained chromophore, which relaxes after a few nanoseconds by a switching of the ionone ring to an essentially planar all-trans conformation. This structural transition of the retinal induces in turn significant conformational changes of the protein backbone, especially in helix VI. Our results suggest a possible molecular mechanism for the early steps of intramolecular signal transduction in a prototypical G-protein-coupled receptor.     

Solid-state 2H NMR spectroscopy of retinal proteins in aligned membranes

Solid-state 2H NMR spectroscopy gives a powerful avenue to investigating the structures of ligands and cofactors bound to integral membrane proteins. For bacteriorhodopsin (bR) and rhodopsin, retinal was site-specifically labeled by deuteration of the methyl groups followed by regeneration of the apoprotein. 2H NMR studies of aligned membrane samples were conducted under conditions where rotational and translational diffusion of the protein were absent on the NMR time scale. The theoretical lineshape treatment involved a static axial distribution of rotating C-C2H3 groups about the local membrane frame, together with the static axial distribution of the local normal relative to the average normal. Simulation of solid-state 2H NMR lineshapes gave both the methyl group orientations and the alignment disorder (mosaic spread) of the membrane stack. The methyl bond orientations provided the angular restraints for structural analysis. In the case of bR the retinal chromophore is nearly planar in the dark- and all-trans light-adapted states, as well upon isomerization to 13-cis in the M state. The C13-methyl group at the "business end" of the chromophore changes its orientation to the membrane upon photon absorption, moving towards W182 and thus driving the proton pump in energy conservation. Moreover, rhodopsin was studied as a prototype for G protein-coupled receptors (GPCRs) implicated in many biological responses in humans. In contrast to bR, the retinal chromophore of rhodopsin has an 11-cis conformation and is highly twisted in the dark state. Three sites of interaction affect the torsional deformation of retinal, viz. the protonated Schiff base with its carboxylate counterion; the C9-methyl group of the polyene; and the beta-ionone ring within its hydrophobic pocket. For rhodopsin, the strain energy and dynamics of retinal as established by 2H NMR are implicated in substituent control of activation. Retinal is locked in a conformation that is twisted in the direction of the photoisomerization, which explains the dark stability of rhodopsin and allows for ultra-fast isomerization upon absorption of a photon. Torsional strain is relaxed in the meta I state that precedes subsequent receptor activation. Comparison of the two retinal proteins using solid-state 2H NMR is thus illuminating in terms of their different biological functions.     

The nature of the primary photochemical events in rhodopsin and isorhodopsin.

The nature of the primary photochemical events in rhodopsin and isorhodopsin is studied by using low temperature actinometry, low temperature absorption spectroscopy, and intermediate neglect of differential overlap including partial single and double configuration interaction (INDO-PSDCI) molecular orbital theory. The principal goal is a better understanding of how the protein binding site influences the energetic, photochemical, and spectroscopic properties of the bound chromophore. Absolute quantum yields for the isorhodopsin (I) to bathorhodopsin (B) phototransformation are assigned at 77 K by using the rhodopsin (R) to bathorhodopsin phototransformation as an internal standard (phi R----B = 0.67). In contrast to rhodopsin photochemistry, isorhodopsin displays a wavelength dependent quantum yield for photochemical generation of bathorhodopsin at 77 K. Measurements at seven wavelengths yielded values ranging from a low of 0.089 +/- 0.021 at 565 nm to a high of 0.168 +/- 0.012 at 440 nm. An analysis of these data based on a variety of kinetic models suggests that the I----B phototransformation encounters a small activation barrier (approximately 0.2 kcal mol-1) associated with the 9-cis----9-trans excited-state torsional-potential surface. The 9-cis retinal chromophore in solution (EPA, 77 K) has the smallest oscillator strength relative to the other isomers: 1.17 (all-trans), 0.98 (9-cis), 1.04 (11-cis), and 1.06 (13-cis). The effect of conformation is quite different for the opsin-bound chromophores. The oscillator strength of the lambda max absorption band of I is observed to be anomalously large (1.11) relative to the lambda max absorption bands of R (0.98) and B (1.07). The wavelength-dependent photoisomerization quantum yields and the anomalous oscillator strength associated with isorhodopsin provide important information on the nature of the opsin binding site. Various models of the binding site were tested by using INDO-PSDCI molecular orbital theory to predict the oscillator strengths of R, B, and I and to calculate the barriers and energy storage associated with the photochemistry of R and I for each model. Our experimental and theoretical investigation leads to the following conclusions: (a) The counterion (abbreviated as CTN) is not intimately associated with the imine proton in R, B, or I. The counterion lies underneath the plane of the chromophore in R and I, and the primary chromophore-counterion electrostatic interactions involve C15-CTN and C13-CTN. These interactions are responsible for the anomalous oscillator strength of I relative to R and B.(ABSTRACT TRUNCATED AT 400 WORDS)     

13C magic-angle spinning NMR studies of bathorhodopsin, the primary photoproduct of rhodopsin.

Magic-angle spinning NMR spectra have been obtained of the bathorhodopsin photointermediate trapped at low temperature (less than 130 K) by using isorhodopsin samples regenerated with retinal specifically 13C-labeled at positions 8, 10, 11, 12, 13, 14, and 15. Comparison of the chemical shifts of the bathorhodopsin resonances with those of an all-trans-retinal protonated Schiff base (PSB) chloride salt show the largest difference (6.2 ppm) at position 13 of the protein-bound retinal. Small differences in chemical shift between bathorhodopsin and the all-trans PSB model compound are also observed at positions 10, 11, and 12. The effects are almost equal in magnitude to those previously observed in rhodopsin and isorhodopsin. Consequently, the energy stored in the primary photoproduct bathorhodopsin does not give rise to any substantial change in the average electron density at the labeled positions. The data indicate that the electronic and structural properties of the protein environment are similar to those in rhodopsin and isorhodopsin. In particular, a previously proposed perturbation near position 13 of the retinal appears not to change its position significantly with respect to the chromophore upon isomerization. The data effectively exclude charge separation between the chromophore and a protein residue as the main mechanism for energy storage in the primary photoproduct and argue that the light energy is stored in the form of distortions of the bathorhodopsin chromophore.     

Conformational similarities in the beta-ionone ring region of the rhodopsin chromophore in its ground state and after photoactivation to the metarhodopsin-I intermediate

High-resolution solid-state NMR methods have been used to analyze the conformation of the chromophore in the late photointermediate metarhodopsin-I, from observation of (13)C nuclei introduced into the beta-ionone ring (at the C16, C17, and C18 methyl groups) and into the adjoining segment of the polyene chain (at C8). Bovine rhodopsin in its native membrane was also regenerated with retinal that was (13)C-labeled close to the 11-Z bond (C20 methyl group) to provide a reporter for optimizing and quantifying the photoconversion to metarhodopsin-I. Indirect photoconversion via the primary intermediate, bathorhodopin, was adopted as the preferred method since approximately 44% conversion to the metarhodopsin-I component could be achieved, with only low levels (approximately 18%) of ground-state rhodopsin remaining. The additional photoproduct, isorhodopsin, was resolved in (13)C spectra from C8 in the chain, at levels of approximately 38%, and was shown using rotational resonance NMR to adopt the 6-s-cis conformation between the ring and the polyene chain. The C8 resonance was not shifted in the metarhodopsin-I spectral component but was strongly broadened, revealing that the local conformation had become less well defined in this segment of the chain. This line broadening slowed rotational resonance exchange with the C17 and C18 ring methyl groups but was accounted for to show that, despite the chain being more relaxed in metarhodopsin-I, its average conformation with respect to the ring was similar to that in the ground state protein. Conformational restraints are also retained for the C16 and C17 methyl groups on photoactivation, which, together with the largely preserved conformation in the chain, argues convincingly that the ring remains with strong contacts in its binding pocket prior to activation of the receptor. Previous conclusions based on photocrosslinking studies are considered in view of the current findings.     

Comparative study on the chromophore binding sites of rod and red-sensitive cone visual pigments by use of synthetic retinal isomers and analogues

A comparative study on the chromophore (retinal) binding sites of the opsin (R-photopsin) from chicken red-sensitive cone visual pigment (iodopsin) and that scotopsin) from bovine rod pigment (rhodopsin) was made by the aid of geometric isomers of retinal (all-trans, 13-cis, 11-cis, 9-cis, and 7-cis) and retinal analogues including fluorinated (14-F, 12-F, 10-F, and 8-F) and methylated (12-methyl) 11-cis-retinals. The stereoselectivity of R-photopsin for the retinal isomers and analogues was almost identical with that of scotopsin, indicating that the shapes of the chromophore binding sites of both opsins are similar, although the former appears to be somewhat more restricted than the latter. The rates of pigment formation from R-photopsin were considerably greater than those from scotopsin. In addition, all the iodopsin isomers and analogues were more susceptible to hydroxylamine than were the rhodopsin ones. These observations suggest that the retinal binding site of iodopsin is located near the protein surface. On the basis of the spectral properties of fluorinated analogues, a polar group in the chromophore binding site of iodopsin as well as rhodopsin was estimated to be located near the hydrogen atom at the C10 position of the retinylidene chromophore. A large difference in wavelength between the absorption maxima of iodopsin and rhodopsin was significantly reduced in the 9-cis and 7-cis pigments. On the assumption that the retinylidene chromophore is anchored rigidly at the alpha-carbon of the lysine residue and loosely at the cyclohexenyl ring, each of the two isomers would have the Schiff-base nitrogen at a position altered from that of the 11-cis pigments.(ABSTRACT TRUNCATED AT 250 WORDS)     

The angles between the C(1)-, C(5)-, and C(9)-methyl bonds of the retinylidene chromophore and the membrane normal increase in the M intermediate of bacteriorhodopsin: direct determination with solid-state (2)H NMR.

The orientations of three methyl bonds of the retinylidene chromophore of bacteriorhodopsin were investigated in the M photointermediate using deuterium solid-state NMR ((2)H NMR). In this key intermediate, the chromophore has a 13-cis, 15-anti conformation and a deprotonated Schiff base. Purple membranes containing wild-type or mutant D96A bacteriorhodopsin were regenerated with retinals specifically deuterated in the methyl groups of either carbon C(1) or C(5) of the beta-ionone ring or carbon C(9) of the polyene chain. Oriented hydrated films were formed by drying concentrated suspensions on glass plates at 86% relative humidity. The lifetime of the M state was increased in the wild-type samples by applying a guanidine hydrochloride solution at pH 9.5 and in the D96A sample by raising the pH. (2)H NMR experiments were performed on the dark-adapted ground state (a 2:1 mixture of 13-cis, 15-syn and all-trans, 15-anti chromophores), the cryotrapped light-adapted state (all-trans, 15-anti), and the cryotrapped M intermediate (13-cis, 15-anti) at -50 degrees C. Bacteriorhodopsin was first completely converted to M under steady illumination of the hydrated films at +5 degrees C and then rapidly cooled to -50 degrees C in the dark. From a tilt series of the oriented sample in the magnetic field and an analysis of the (2)H NMR line shapes, the angles between the individual C-CD(3) bonds and the membrane normal could be determined even in the presence of a substantial degree of orientational disorder. While only minor differences were detected between dark- and light-adapted states, all three angles increase in the M state. This is consistent with an upward movement of the C(5)-C(13) part of the polyene chain toward the cytoplasmic surface or with increased torsional strain. The C(9)-CD(3) bond shows the largest orientational change of 7 degrees in M. This reorientation of the chromophore in the binding pocket provides direct structural support for previous suggestions (based on spectroscopic evidence) for a steric interaction in M between the C(9)-methyl group and Trp 182 in helix F.     

Crystallographic analysis of the primary photochemical reaction of squid rhodopsin

Visual signal transduction is initiated by the photoisomerization of 11-cis retinal upon rhodopsin ligation. Unlike vertebrate rhodopsin, which interacts with Gt-type G-protein to stimulate the cyclic GMP signaling pathway, invertebrate rhodopsin interacts with Gq-type G-protein to stimulate a signaling pathway that is based on inositol 1,4,5-triphosphate. Since the inositol 1,4,5-triphosphate signaling pathway is utilized by mammalian nonvisual pigments and a large number of G-protein-coupled receptors, it is important to elucidate how the activation mechanism of invertebrate rhodopsin differs from that of vertebrate rhodopsin. Previous crystallographic studies of squid and bovine rhodopsins have shown that there is a profound difference in the structures of the retinal-binding pockets of these photoreceptors. Here, we report the crystal structures of all-trans bathorhodopsin (Batho; the first photoreaction intermediate) and the artificial 9-cis isorhodopsin (Iso) of squid rhodopsin. Upon the formation of Batho, the central moiety of the retinal was observed to move largely towards the cytoplasmic side, while the Schiff base and the ionone ring underwent limited movements (i.e., the all-trans retinal in Batho took on a right-handed screwed configuration). Conversely, the 9-cis retinal in Iso took on a planar configuration. Our results suggest that the light energy absorbed by squid rhodopsin is mostly converted into the distortion energy of the retinal polyene chain and surrounding residues.     

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.     

Inherent Instability of the Retinitis Pigmentosa P23H Mutant Opsin

The P23H opsin mutation is the most common cause of autosomal dominant retinitis pigmentosa. Even though the pathobiology of the resulting retinal degeneration has been characterized in several animal models, its complex molecular mechanism is not well understood. Here, we expressed P23H bovine rod opsin in the nervous system of Caenorhabditis elegans. Expression was low due to enhanced protein degradation. The mutant opsin was glycosylated, but the polysaccharide size differed from that of the normal protein. Although P23H opsin aggregated in the nervous system of C. elegans, the pharmacological chaperone 9-cis-retinal stabilized it during biogenesis, producing a variant of rhodopsin called P23H isorhodopsin. In vitro, P23H isorhodopsin folded correctly, formed the appropriate disulfide bond, could be photoactivated but with reduced sensitivity, and underwent Meta II decay at a rate similar to wild type isorhodopsin. In worm neurons, P23H isorhodopsin initiated phototransduction by coupling with the endogenous G_i/o signaling cascade that induced loss of locomotion. Using pharmacological interventions affecting protein synthesis and degradation, we showed that the chromophore could be incorporated either during or after mutant protein translation. However, regeneration of P23H isorhodopsin with chromophore was significantly slower than that of wild type isorhodopsin. This effect, combined with the inherent instability of P23H rhodopsin, could lead to the structural cellular changes and photoreceptor death found in autosomal dominant retinitis pigmentosa. These results also suggest that slow regeneration of P23H rhodopsin could prevent endogenous chromophore-mediated stabilization of rhodopsin in the retina.     

A comparative study of the infrared difference spectra for octopus and bovine rhodopsins and their bathorhodopsin photointermediates

Fourier-transform infrared difference spectroscopy has been used to detect the vibrational modes in the chromophore and protein that change in position and intensity between octopus rhodopsin and its photoproducts formed at low temperature (85 K), bathorhodopsin and isorhodopsin. The infrared difference spectra between octopus rhodopsin and octopus bathorhodopsin, octopus bathorhodopsin and octopus isorhodopsin, and octopus isorhodopsin and octopus rhodopsin are compared to analogous difference spectra for the well-studied bovine pigments, in order to understand the similarities in pigment structure and photochemical processes between the vertebrate and invertebrate systems. The structure-sensitive fingerprint region of the infrared spectra for octopus bathorhodopsin shows strong similarities to spectra of both all-trans-retinal and bovine bathorhodopsin, thus confirming chemical extraction data that suggest that octopus bathorhodopsin contains an all-trans-retinal chromophore. In contrast, we find dramatic differences in the hydrogen out-of-plane modes of the two bathorhodopsins, and in the fingerprint lines of the rhodopsins and isorhodopsins for the two pigments. These observations suggest that while the primary effect of light in the octopus rhodopsin system, as in the bovine rhodopsin system, is 11-cis/11-trans isomerization, the protein-chromophore interactions for the two systems are quite different. Finally, striking similarities and differences in infrared lines attributable to changes in amino acid residues in the opsin are found between the two pigment systems. They suggest that no carboxylic acid or tyrosine residues are affected in the initial changes of light-energy transduction in octopus rhodopsin. Comparing the amino acid sequences for octopus and bovine pigments also allows us to suggest that the carboxylic acid residues altered in the bovine transitions are Glu-122 and/or Glu-134.     

Retinal analog restoration of photophobic responses in a blind Chlamydomonas reinhardtii mutant. Evidence for an archaebacterial like chromophore in a eukaryotic rhodopsin.

The strain CC-2359 of the unicellular eukaryotic alga Chlamydomonas reinhardtii originally described as a low pigmentation mutant is found to be devoid of photophobic stop responses to photostimuli over a wide range of light intensities. Photophobic responses of the mutant are restored by exogenous addition of all-trans retinal. We have combined computer-based cell-tracking and motion analysis with retinal isomer and retinal analog reconstitution of CC-2359 to investigate properties of the photophobic response receptor. Most rapid and most complete reconstitution is obtained with all-trans retinal compared to 13-cis, 11-cis, and 9-cis retinal. An analog locked by a carbon bridge in a 6-s-trans conformation reconstitutes whereas the corresponding 6-s-cis locked analog does not. Retinal analogs prevented from isomerization around the 13-14 double bond by a five-membered ring in the polyene chain (locked in either the 13-trans or 13-cis configuration) do not restore the response, but enter the chromophore binding pocket as evidenced by their inhibition of all-trans retinal regeneration of the response. Results of competition experiments between all-trans and each of the 13-locked analogs fit a model in which each chromophore exhibits reversible binding to the photoreceptor apoprotein. A competitive inhibition scheme closely fits the data and permits calculation of apparent dissociation constants for the in vivo reconstitution process of 2.5 x 10(-11) M, 5.2 x 10(-10) M, and 5.4 x 10(-9) M, for all-trans, 13-trans-locked and 13-cis-locked analogs, respectively. The chromophore requirement for the trans configuration and 6-s-trans conformation, and the lack of signaling function from analogs locked at the 13 position, are characteristic of archaebacterial rhodopsins, rather than the previously studied eukaryotic rhodopsins (i.e., visual pigments).     

Spectral tuning in salamander visual pigments studied with dihydroretinal chromophores.

In visual pigments, opsin proteins regulate the spectral absorption of a retinal chromophore by mechanisms that change the energy level of the excited electronic state relative to the ground state. We have studied these mechanisms by using photocurrent recording to measure the spectral sensitivities of individual red rods and red (long-wavelength-sensitive) and blue (short-wavelength-sensitive) cones of salamander before and after replacing the native 3-dehydro 11-cis retinal chromophore with retinal analogs: 11-cis retinal, 3-dehydro 9-cis retinal, 9-cis retinal, and 5,6-dihydro 9-cis retinal. The protonated Schiff's bases of analogs with unsaturated bonds in the ring had broader spectra than the same chromophores bound to opsins. Saturation of the bonds in the ring reduced the spectral bandwidths of the protonated Schiff's bases and the opsin-bound chromophores and made them similar to each other. This indicates that torsion of the ring produces spectral broadening and that torsion is limited by opsin. Saturating the 5,6 double bond in retinal reduced the perturbation of the chromophore by opsin in red and in blue cones but not in red rods. Thus an interaction between opsin and the chromophoric ring shifts the spectral maxima of the red and blue cone pigments, but not that of the red rod pigment.     

Assignment of fingerprint vibrations in the resonance Raman spectra of rhodopsin, isorhodopsin, and bathorhodopsin: implications for chromophore structure and environment

13C- and 2H-labeled retinal derivatives have been used to assign normal modes in the 1100-1300-cm-1 fingerprint region of the resonance Raman spectra of rhodopsin, isorhodopsin, and bathorhodopsin. On the basis of the 13C shifts, C8-C9 stretching character is assigned at 1217 cm-1 in rhodopsin, at 1206 cm-1 in isorhodopsin, and at 1214 cm-1 in bathorhodopsin. C10-C11 stretching character is localized at 1098 cm-1 in rhodopsin, at 1154 cm-1 in isorhodopsin, and at 1166 cm-1 in bathorhodopsin. C14-C15 stretching character is found at 1190 cm-1 in rhodopsin, at 1206 cm-1 in isorhodopsin, and at 1210 cm-1 in bathorhodopsin. C12-C13 stretching character is much more delocalized, but the characteristic coupling with the C14H rock allows us to assign the "C12-C13 stretch" at approximately 1240 cm-1 in rhodopsin, isorhodopsin, and bathorhodopsin. The insensitivity of the C14-C15 stretching mode to N-deuteriation in all three pigments demonstrates that each contains a trans (anti) protonated Schiff base bond. The relatively high frequency of the C10-C11 mode of bathorhodopsin demonstrates that bathorhodopsin is s-trans about the C10-C11 single bond. This provides strong evidence against the model of bathorhodopsin proposed by Liu and Asato [Liu, R., & Asato, A. (1985) Proc. Natl. Acad. Sci. U.S.A. 82, 259], which suggests a C10-C11 s-cis structure. Comparison of the fingerprint modes of rhodopsin (1098, 1190, 1217, and 1239 cm-1) with those of the 11-cis-retinal protonated Schiff base in methanol (1093, 1190, 1217, and 1237 cm-1) shows that the frequencies of the C-C stretching modes are largely unperturbed by protein binding. In particular, the invariance of the C14-C15 stretching mode at 1190 cm-1 does not support the presence of a negative protein charge near C13 in rhodopsin. In contrast, the frequencies of the C8-C9 and C14-C15 stretches of bathorhodopsin and the C10-C11 and C14-C15 stretches of isorhodopsin are significantly altered by protein binding. The implications of these observations for the mechanism of wavelength regulation in visual pigments and energy storage in bathorhodopsin are discussed.     

Raman microscope and quantum yield studies on the primary photochemistry of A2-visual pigments.

The 77-K resonance Raman vibrational spectrum of intact goldfish rod photoreceptors containing 3,4-dehydro (A2) retinal is dominated by scattering from the 9-cis component of the steady state at all excitation wavelengths. Intact goldfish photoreceptors were regenerated with an A1-retinal chromophore to determine whether this behavior is caused by the protein or the chromophore. The resulting Raman spectrum was typical of an A1-pigment exhibiting significant scattering from all three components of the steady state: rhodopsin, bathorhodopsin, and isorhodopsin. Furthermore, regeneration of bovine opsin with A2-retinal produces a characteristic "A2-Raman spectrum" that is dominated by scattering from the 9-cis pigment. We conclude that the differences between the Raman spectra of the A1-and A2-pigments are caused by some intrinsic difference in the photochemical properties of the retinal chromophores. To quantitate these observations, the 77-K adsorption spectra and the photochemical quantum yields (phi) of the native A2-goldfish and the regenerated A2-bovine pigments were measured. In the goldfish A2-pigment, the value of phi 4 (9-cis----trans) is 0.05; phi 3 (trans----9-cis) is 0.10; and phi 2 (trans----11-cis) is 0.35. By contrast, in the bovine A1-pigment, these quantum yields are 0.10, 0.053, and 0.50, respectively. The reduced value of phi 4 and the increased value of phi 3 in the goldfish pigment confirms that the 9-cis isomer is photochemically more stable in A2-pigments.     

Structure and protein environment of the retinal chromophore in light- and dark-adapted bacteriorhodopsin studied by solid-state NMR

Our previous solid-state 13C NMR studies on bR have been directed at characterizing the structure and protein environment of the retinal chromophore in bR568 and bR548, the two components of the dark-adapted protein. In this paper, we extend these studies by presenting solid-state NMR spectra of light-adapted bR (bR568) and examining in more detail the chemical shift anisotropy of the retinal resonances near the ionone ring and Schiff base. Magic angle spinning (MAS) 13C NMR spectra were obtained of bR568, regenerated with retinal specifically 13C labeled at positions 12-15, which allowed assignment of the resonances observed in the dark-adapted bR spectrum. Of particular interest are the assignments of the 13C-13 and 13C-15 resonances. The 13C-15 chemical resonance for bR568 (160.0 ppm) is upfield of the 13C-15 resonance for bR548 (163.3 ppm). This difference is attributed to a weaker interaction between the Schiff base and its associated counterion in bR568. The 13C-13 chemical shift for bR568 (164.8 ppm) is close to that of the all-trans-retinal protonated Schiff base (PSB) model compound (approximately 162 ppm), while the 13C-13 resonance for bR548 (168.7 ppm) is approximately 7 ppm downfield of that of the 13-cis PSB model compound. The difference in the 13C-13 chemical shift between bR568 and bR548 is opposite that expected from the corresponding 15N chemical shifts of the Schiff base nitrogen and may be due to conformational distortion of the chromophore in the C13 = C14-C15 bonds.(ABSTRACT TRUNCATED AT 250 WORDS)     

FTIR study of the photoisomerization processes in the 13-cis and all-trans forms of Anabaena sensory rhodopsin at 77 K

Archaeal-type rhodopsins can accommodate either all-trans- or 13-cis,15-syn-retinal in their chromophore binding site in the dark, but only the former isomer is functionally important. In contrast, Anabaena sensory rhodopsin (ASR), an archaeal-type rhodopsin found in eubacteria, exhibits a photochromic interconversion of both forms, suggesting that ASR functions as a photosensor which interacts with its 14 kDa soluble transducer differently in the all-trans and 13-cis,15-syn forms. In this study, we applied low-temperature Fourier transform infrared (FTIR) spectroscopy to the 13-cis,15-syn form of ASR (13C-ASR) at 77 K and compared the local structure around the chromophore and its structural changes upon retinal photoisomerization with those of the all-trans form (AT-ASR) [Furutani, Y., Kawanabe, A., Jung, K. H., and Kandori, H. (2005) Biochemistry 44, 12287-12296]. By use of [zeta-15N]lysine-labeled ASR, we identified the N-D stretching vibrations of the Schiff base (in D2O) at 2165 cm(-1) for 13C-ASR and at 2163 and 2125 cm(-1) for AT-ASR. The frequencies indicate strong hydrogen bonds of the Schiff base with a water molecule for both 13C-ASR and AT-ASR. In contrast, the N-D stretching vibration appears at 2351 cm(-1) and at 2483 cm(-1) for the K states of 13C-ASR (13C-ASR(K)) and AT-ASR (AT-ASR(K)), respectively, indicating that the Schiff base still forms a hydrogen bond in 13C-ASR(K). Rotational motion of the Schiff base upon retinal isomerization is probably smaller for 13C-ASR than for AT-ASR, the latter altering hydrogen bonding of the Schiff base similar to bacteriorhodopsin (BR), a light-driven proton pump. Appearance of several hydrogen-out-of-plane vibrations and amide I vibrations in 13C-ASR(K), but not in AT-ASR(K), suggests that structural changes are distributed widely along the polyene chain for 13C-ASR. On the other hand, retinal photoisomerization in AT-ASR breaks the hydrogen bond of the Schiff base, and localized structural changes in the Schiff base region are induced.     

Studies on cephalopod rhodopsin: photoisomerization of the chromophore.

Photoisomerization of the chromophore of squid rhodopsin is dependent upon the irradiation temperature. Above 0 degrees C, only 11-cis in equilibrium all-trans reaction proceeds and the all-trans leads to 9-cis reaction is limited to extremely low efficiency. At liquid nitrogen temperature, 11 cis in equilibrium all-trans in equilibrium 9-cis reaction takes place. At intermediary low temperatures (-80 degrees C to -15 degrees C) another isomer of retinal may be produced by the irradiation, which forms a pigment having an absorbance maximum at 465 nm (P-465). The formation of P-465 decreases remarkably in the narrow temperature range from -30 degrees C to 0 degrees C where mesorhodopsin converts to metarhodopsin. Medsorhodopsin is quite different from metarhodopsin in the photoisomerization of the chromophore because P-465 is produced from the former but not from the latter. No P-465 is produced both at liquid nitrogen temperature and above 0 degrees C. P-465 is more labile than any of the other photoproducts so far known, that is isorhodopsin, alkaline and acid metarhodopsins. P-465 is converted to metarhodopsin by irradiation.