Formation of Meta III during the decay of activated rhodopsin proceeds via Meta I and not via Meta II

Thermal isomerization of the retinal Schiff base C=N double bond is known to trigger the decay of rhodopsin's Meta I/Meta II photoproduct equilibrium to the inactive Meta III state [Vogel, R., Siebert, F., Mathias, G., Tavan, P., Fan, G., and Sheves, M. (2003) Biochemistry 42, 9863-9874]. Previous studies have indicated that the transition to Meta III does not occur under conditions that strongly favor the active state Meta II but requires a residual amount of Meta I in the initial photoproduct equilibrium. In this study we show that the triggering event, the thermal isomerization of the protonated Schiff base, is independent of the presence of Meta II and occurs even under conditions where the transition to Meta II is completely prevented. We have examined two examples in which the transitions from Lumi to Meta I or from Meta I to Meta II are blocked. This was achieved using dry films of rhodopsin and rhodopsin reconstituted into rather rigid lipid bilayers. In both cases, the resulting fully inactive room temperature photoproducts decay specifically by thermal isomerization of the protonated Schiff base C=N double bond to an all-trans 15-syn chromophore isomer, corresponding to that of Meta III. This thermal isomerization becomes less efficient as the conformation of the respective photoproduct approaches that of Meta II and is fully absent in a pure Meta II state. These results indicate that the decay of the Meta I/Meta II photoproduct equilibrium to Meta III proceeds via Meta I and not via 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.     

Rhodopsin with 11-cis-locked chromophore is capable of forming an active state photoproduct

The visual pigment rhodopsin is characterized by an 11-cis retinal chromophore bound to Lys-296 via a protonated Schiff base. Following light absorption the C(11)=C(12) double bond isomerizes to trans configuration and triggers protein conformational alterations. These alterations lead to the formation of an active intermediate (Meta II), which binds and activates the visual G protein, transducin. We have examined by UV-visible and Fourier transform IR spectroscopy the photochemistry of a rhodopsin analogue with an 11-cis-locked chromophore, where cis to trans isomerization around the C(11)=C(12) double bond is prevented by a 6-member ring structure (Rh(6.10)). Despite this lock, the pigment was found capable of forming an active photoproduct with a characteristic protein conformation similar to that of native Meta II. This intermediate is further characterized by a protonated Schiff base and protonated Glu-113, as well as by its ability to bind a transducin-derived peptide previously shown to interact efficiently with native Meta II. The yield of this active photointermediate is pH-dependent and decreases with increasing pH. This study shows that with the C(11)=C(12) double bond being locked, isomerization around the C(9)=C(10) or the C(13)=C(14) double bonds may well lead to an activation of the receptor. Additionally, prolonged illumination at pH 7.5 produces a new photoproduct absorbing at 385 nm, which, however, does not exhibit the characteristic active protein conformation.     

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.     

Solid-state NMR analysis of ligand--receptor interactions reveals an induced misfit in the binding site of isorhodopsin

Rhodopsin is the photosensitive protein of the rod photoreceptor in the vertebrate retina and is a paradigm for the superfamily of G-protein-coupled receptors (GPCRs). Natural rhodopsin contains an 11-cis-retinylidene chromophore. We have prepared the 9-cis analogue isorhodopsin in a natural membrane environment using uniformly (13)C-enriched 9-cis retinal. Subsequently, we have determined the complete (1)H and (13)C assignments with ultra-high field solid-state magic angle spinning NMR. The 9-cis substrate conforms to the opsin binding pocket in isorhodopsin in a manner very similar to that of the 11-cis form in rhodopsin, but the NMR data reveal an improper fit of the 9-cis chromophore in this binding site. We introduce the term "induced misfit" to describe this event. Downfield proton NMR ligation shifts (Deltasigma(lig)(H) > 1 ppm) are observed for the 16,17,19-H and nearby protons of the ionone ring and for the 9-methyl protons. They provide converging evidence for global, nonspecific steric interactions between the chromophore and protein, and contrast with the specific interactions over the entire ionone ring and its substituents detected for rhodopsin. The Deltasigma(lig)(C) pattern of the polyene chain confirms the positive charge delocalization in the polyene associated with the protonation of the Schiff base nitrogen. In line with the misalignment of the ionone ring, an additional and anomalous perturbation of the (13)C response is detected in the region of the 9-cis bond. This provides evidence for strain in the isomerization region of the polyene and supports the hypothesis that perturbation of the conjugation around the cis bond induced by the protein environment assists the selective photoisomerization.     

Fourier-transform infrared difference spectroscopy of rhodopsin and its photoproducts at low temperature

Fourier-transform infrared difference spectroscopy has been used to detect the vibrational modes in the chromophore and protein that change in position or intensity between rhodopsin and the photoproducts formed at low temperature (70 K), bathorhodopsin and isorhodopsin. A method has been developed to obtain infrared difference spectra between rhodopsin and bathorhodopsin, bathorhodopsin and isorhodopsin, and rhodopsin and isorhodopsin. To aid in the identification of the vibrational modes, we performed experiments on deuterated and hydrated films of native rod outer segments and rod outer segments regenerated with either retinal containing 13C at carbon 15 or 15-deuterioretinal. Our infrared measurements provide independent verification of the resonance Raman result that the retinal in bathorhodopsin is distorted all-trans. The positions of the C = N stretch in the deuterated pigment and the deuterated pigments regenerated with 11-cis-15-deuterioretinal or 11-cis-retinal containing 13C at carbon 15 are indicative that the Schiff-base linkage is protonated in rhodopsin, bathorhodopsin, and isorhodopsin. Furthermore, the C = N stretching frequency occurs at the same position in all three species. The data indicate that the protonated Schiff base has a C = N trans conformation in all three species. Finally, we present evidence that, even in these early stages of the rhodopsin photosequence, changes are occurring in the opsin and perhaps the associated lipids.     

Structure of the retinal chromophore in 7,9-dicis-rhodopsin

Bovine rhodopsin was bleached and regenerated with 7,9-dicis-retinal to form 7,9-dicis-rhodopsin, which was purified on a concanavalin A affinity column. The absorption maximum of the 7,9-dicis pigment is 453 nm, giving an opsin shift of 1600 cm-1 compared to 2500 cm-1 for 11-cis-rhodopsin and 2400 cm-1 for 9-cis-rhodopsin. Rapid-flow resonance Raman spectra have been obtained of 7,9-dicis-rhodopsin in H2O and D2O at room temperature. The shift of the 1654-cm-1 C = N stretch to 1627 cm-1 in D2O demonstrates that the Schiff base nitrogen is protonated. The absence of any shift in the 1201-cm-1 mode, which is assigned as the C14-C15 stretch, or of any other C-C stretching modes in D2O indicates that the Schiff base C = N configuration is trans (anti). Assuming that the cyclohexenyl ring binds with the same orientation in 7,9-dicis-, 9-cis-, and 11-cis-rhodopsins, the presence of two cis bonds requires that the N-H bond of the 7,9-dicis chromophore points in the opposite direction from that in the 9-cis or 11-cis pigment. However, the Schiff base C = NH+ stretching frequency and its D2O shift in 7,9-dicis-rhodopsin are very similar to those in 11-cis- and 9-cis-rhodopsin, indicating that the Schiff base electrostatic/hydrogen-bonding environments are effectively the same. The C = N trans (anti) Schiff base geometry of 7,9-dicis-rhodopsin and the insensitivity of its Schiff base vibrational properties to orientation are rationalized by examining the binding site specificity with molecular modeling.     

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.     

Investigations of the rhodopsin/Meta I and rhodopsin/Meta II transitions of bovine rod outer segments by means of kinetic infrared spectroscopy

We have applied our recently developed technique of flash induced kinetic infrared spectroscopy to the rhodopsin/Meta I and rhodopsin/Meta II transitions. Features of the infrared spectrum reflecting the C=C-vibration and the isomeric form of the chromophore are in agreement with resonant Raman experiments. Different results are obtained for the C=N-vibration of the Schiff base retinal opsin link. They are interpreted in terms of a Schiff base protonated via an hydrogen bond. A proton transfer in the excited state is suggested to explain the deviating results. In addition we have obtained spectral changes which cannot be attributed to molecular changes in the chromophore. We assume that these spectral features reflect molecular events in the protein part of rhodopsin.     

Signaling states of rhodopsin. Formation of the storage form,metarhodopsin III,from active metarhodopsin II

Vertebrate rhodopsin consists of the apoprotein opsin and the chromophore 11-cis-retinal covalently linked via a protonated Schiff base. Upon photoisomerization of the chromophore to all-trans-retinal, the retinylidene linkage hydrolyzes, and all-trans-retinal dissociates from opsin. The pigment is eventually restored by recombining with enzymatically produced 11-cis-retinal. All-trans-retinal release occurs in parallel with decay of the active form, metarhodopsin (Meta) II, in which the original Schiff base is intact but deprotonated. The intermediates formed during Meta II decay include Meta III, with the original Schiff base reprotonated, and Meta III-like pseudo-photoproducts. Using an intrinsic fluorescence assay, Fourier transform infrared spectroscopy, and UV-visible spectroscopy, we investigated Meta II decay in native rod disk membranes. Up to 40% of Meta III is formed without changes in the intrinsic Trp fluorescence and thus without all-trans-retinal release. NADPH, a cofactor for the reduction of all-trans-retinal to all-trans-retinol, does not accelerate Meta II decay nor does it change the amount of Meta III formed. However, Meta III can be photoconverted back to the Meta II signaling state. The data are described by two quasi-irreversible pathways, leading in parallel into Meta III or into release of all-trans-retinal. Therefore, Meta III could be a form of rhodopsin that is stored away, thus regulating photoreceptor regeneration.     

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.     

Light-stable rhodopsin. I. A rhodopsin analog reconstituted with a nonisomerizable 11-cis retinal derivative.

With the aim of preparing a light-stable rhodopsin-like pigment, an analog, II, of 11-cis retinal was synthesized in which isomerization of the C11-C12 cis-double bond is blocked by a cyclohexene ring built around the C10 to C13-methyl. The analog II formed a rhodopsin-like pigment (rhodopsin-II) with opsin expressed in COS-1 cells and with opsin from rod outer segments. The rate of rhodopsin-II formation from II and opsin was approximately 10 times slower than that of rhodopsin from 11-cis retinal and opsin. After solubilization in dodecyl maltoside and immunoaffinity purification, rhodopsin-II displayed an absorbance ratio (A280nm/A512nm) of 1.6, virtually identical with that of rhodopsin. Acid denaturation of rhodopsin-II formed a chromophore with lambda max, 452 nm, characteristic of protonated retinyl Schiff base. The ground state properties of rhodopsin-II were similar to those of rhodopsin in extinction coefficient (41,200 M-1 cm-1) and opsin-shift (2600 cm-1). Rhodopsin-II was stable to hydroxylamine in the dark, while light-dependent bleaching by hydroxylamine was slowed by approximately 2 orders of magnitude relative to rhodopsin. Illumination of rhodopsin-II for 10 s caused approximately 3 nm blue-shift and 3% loss of visible absorbance. Prolonged illumination caused a maximal blue-shift up to approximately 20 nm and approximately 40% loss of visible absorbance. An apparent photochemical steady state was reached after 12 min of illumination. Subsequent acid denaturation indicated that the retinyl Schiff base linkage was intact. A red-shift (approximately 12 nm) in lambda max and a 45% recovery of visible absorbance was observed after returning the 12-min illuminated pigment to darkness. Rhodopsin-II showed marginal light-dependent transducin activation and phosphorylation by rhodopsin kinase.     

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.     

Crystal structure of the 13-cis isomer of bacteriorhodopsin in the dark-adapted state

The atomic structure of the trans isomer of bacteriorhodopsin was determined previously by using a 3D crystal belonging to the space group P622. Here, a structure is reported for another isomer with the 13-cis, 15-syn retinal in a dark-adapted crystal. Structural comparison of the two isomers indicates that retinal isomerization around the C13[double bond]C14 and the C15[double bond]N bonds is accompanied by noticeable displacements of a few residues in the vicinity of the retinal Schiff base and small re-arrangement of the hydrogen-bonding network in the proton release channel. On the other hand, aromatic residues surrounding the retinal polyene chain were found to scarcely move during the dark/light adaptation. This result suggests that variation in the structural rigidity within the retinal-binding pocket is one of the important factors ensuring the stereospecific isomerization of retinal.     

Control of the pump cycle in bacteriorhodopsin: mechanisms elucidated by solid-state NMR of the D85N mutant.

By varying the pH, the D85N mutant of bacteriorhodopsin provides models for several photocycle intermediates of the wild-type protein in which D85 is protonated. At pH 10.8, NMR spectra of [zeta-(15)N]lys-, [12-(13)C]retinal-, and [14,15-(13)C]retinal-labeled D85N samples indicate a deprotonated, 13-cis,15-anti chromophore. On the other hand, at neutral pH, the NMR spectra of D85N show a mixture of protonated Schiff base species similar to that seen in the wild-type protein at low pH, and more complex than the two-state mixture of 13-cis,15-syn, and all-trans isomers found in the dark-adapted wild-type protein. These results lead to several conclusions. First, the reversible titration of order in the D85N chromophore indicates that electrostatic interactions have a major influence on events in the active site. More specifically, whereas a straight chromophore is preferred when the Schiff base and residue 85 are oppositely charged, a bent chromophore is found when both the Schiff base and residue 85 are electrically neutral, even in the dark. Thus a "bent" binding pocket is formed without photoisomerization of the chromophore. On the other hand, when photoisomerization from the straight all-trans,15-anti configuration to the bent 13-cis,15-anti does occur, reciprocal thermodynamic linkage dictates that neutralization of the SB and D85 (by proton transfer from the former to the latter) will result. Second, the similarity between the chromophore chemical shifts in D85N at alkaline pH and those found previously in the M(n) intermediate of the wild-type protein indicate that the latter has a thoroughly relaxed chromophore like the subsequent N intermediate. By comparison, indications of L-like distortion are found for the chromophore of the M(o) state. Thus, chromophore strain is released in the M(o)-->M(n) transition, probably coincident with, and perhaps instrumental to, the change in the connectivity of the Schiff base from the extracellular side of the membrane to the cytoplasmic side. Because the nitrogen chemical shifts of the Schiff base indicate interaction with a hydrogen-bond donor in both M states, it is possible that a water molecule travels with the Schiff base as it switches connectivity. If so, the protein is acting as an inward-driven hydroxyl pump (analogous to halorhodopsin) rather than an outward-driven proton pump. Third, the presence of a significant C [double bond] N syn component in D85N at neutral pH suggests that rapid deprotonation of D85 is necessary at the end of the wild-type photocycle to avoid the generation of nonfunctional C [double bond] N syn species.     

Chromophore structure in bacteriorhodopsin's N intermediate: implications for the proton-pumping mechanism

By elevating the pH to 9.5 in 3 M KCl, the concentration of the N intermediate in the bacteriorhodopsin photocycle has been enhanced, and time-resolved resonance Raman spectra of this intermediate have been obtained. Kinetic Raman measurements show that N appears with a half-time of 4 +/- 2 ms, which agrees satisfactorily with our measured decay time of the M412 intermediate (2 +/- 1 ms). This argues that M412 decays directly to N in the light-adapted photocycle. The configuration of the chromophore about the C13 = C14 bond was examined by regenerating the protein with [12,14-2H]retinal. The coupled C12-2H + C14-2H rock at 946 cm-1 demonstrates that the chromophore in N is 13-cis. The shift of the 1642-cm-1 Schiff base stretching mode to 1618 cm-1 in D2O indicates that the Schiff base linkage to the protein is protonated. The insensitivity of the 1168-cm-1 C14-C15 stretching mode to N-deuteriation establishes a C = N anti (trans) Schiff base configuration. The high frequency of the C14-C15 stretching mode as well as the frequency of the 966-cm-1 C14-2H-C15-2H rocking mode shows that the chromophore is 14-s-trans. Thus, N contains a 13-cis, 14-s-trans, 15-anti protonated retinal Schiff base.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Resonance Raman spectroscopy of octopus rhodopsin and its photoproducts

We report here the resonance Raman spectra of octopus rhodopsin and its photoproducts, bathorhodopsin and acid metarhodopsin. These studies were undertaken in order to make comparisons with the well-studied bovine pigments, so as to understand the similarities and the differences in pigment structure and photochemical processes between vertebrates and invertebrates. The flow method was used to obtain the Raman spectrum of rhodopsin at 13 degrees C. The bathorhodopsin spectrum was obtained by computer subtraction of the spectra containing different photostationary mixtures of rhodopsin, isorhodopsin, hypsorhodopsin, and bathorhodopsin, obtained at 12 K using the pump-probe technique and from measurements at 80 K. Like their bovine counterparts, the Schiff base vibrational mode appears at approximately 1660 cm-1 in octopus rhodopsin and the photoproducts, bathorhodopsin and acid metarhodopsin, suggesting a protonated Schiff base linkage between the chromophore and the protein. Differences between the Raman spectra of octopus rhodopsin and bathorhodopsin indicate that the formation of bathorhodopsin is associated with chromophore isomerization. This inference is substantiated by the chromophore chemical extraction data which show that, like the bovine system, octopus rhodopsin is an 11-cis pigment, while the photoproducts contain an all-trans pigment, in agreement with previous work. The octopus rhodopsin and bathorhodopsin spectra show marked differences from their bovine counterparts in other respects, however. The differences are most dramatic in the structure-sensitive fingerprint and the HOOP regions. Thus, it appears that although the two species differ in the specific nature of the chromophore-protein interactions, the general process of visual transduction is the same.     

all-trans-retinoids and dihydroretinoids as probes of the role of chromophore structure in rhodopsin activation

The absorption of a photon of light by rhodopsin results in the cis to trans isomerization of the 11-cis-retinal Schiff base chromophore. In the studies reported here, an attempt is made to determine the mechanism of the energization of rhodopsin as it relates to the chemistry of the isomerization process and the geometrical state of the chromophore. Studies were performed with vitamin A analogues to probe this mechanism. Both 11-cis-7,8-dihydroretinal and 9-cis-7,8-dihydroretinal form bleachable pigments when combined with opsin. Photolysis of these pigments in the presence of G-protein results in the activation of the latter as revealed by its GTPase activity. Phosphodiesterase is also activated when it is included in the incubation. Therefore, the possibility that rhodopsin is energized by mechanisms involving photochemically induced charge transfer from the protonated Schiff base to the beta-ionone ring can be discarded. Further studies were conducted with all-trans-vitamin A derivatives to determine if these compounds can form the GTPase-activating state R*, a situation that is possible, in principle, by microscopic reversibility. Neither all-trans-retinal nor its oxime, when incubated with bovine opsin in the dark, caused activation of the GTPase, requiring at least a 5 kcal/mol energy gap between them. Furthermore, stoichiometric adducts of all-trans-retinoids and opsin were also unable to mediate activation of the GTPase. Since both all-trans-15,16-dihydroretinylopsin and all-trans-retinoylopsin possess an all-trans-retinoid permanently adducted to opsin, it can be concluded that the all-trans-retinoid chromophore-opsin linkage may be necessary but not sufficient to achieve activation of the visual pigment.