Photolysis intermediates of the artificial visual pigment cis-5,6-dihydro-isorhodopsin

Residue-Residue Mutual Work Analysis of Retinal-Opsin Interaction in Rhodopsin: Implications for Protein-Ligand Binding

Energetic contributions at the single-residue level for retinal-opsin interactions in rhodopsin were studied by combining molecular dynamics simulations, transition path sampling, and a newly developed energy decomposition approach. The virtual work at an infinitesimal time interval was decomposed into the work components on one residue due to its interaction with another residue, which were then averaged over the transition path ensemble along a proposed reaction coordinate. Such residue-residue mutual work analysis on 62 residues within the active center of rhodopsin resulted in a very sparse interaction matrix, which is generally not symmetric but antisymmetric to some extent. Fourteen residues were identified to be major players in retinal relaxation along a plausible pathway from bathorhodopsin to the blue-shifted intermediate, which is in good agreement with an existing NMR study. Based on the matrix of mutual work, a comprehensive network was constructed to provide detailed insights into the chromophore-protein interaction from a viewpoint of energy flow.

Low-Temperature Trapping of Photointermediates of the Rhodopsin E181Q Mutant

Three active-site components in rhodopsin play a key role in the stability and function of the protein: 1) the counter-ion residues which stabilize the protonated Schiff base, 2) water molecules, and 3) the hydrogen-bonding network. The ionizable residue Glu-181, which is involved in an extended hydrogen-bonding network with Ser-186, Tyr-268, Tyr-192, and key water molecules within the active site of rhodopsin, has been shown to be involved in a complex counter-ion switch mechanism with Glu-113 during the photobleaching sequence of the protein. Herein, we examine the photobleaching sequence of the E181Q rhodopsin mutant by using cryogenic UV-visible spectroscopy to further elucidate the role of Glu-181 during photoactivation of the protein. We find that lower temperatures are required to trap the early photostationary states of the E181Q mutant compared to native rhodopsin. Additionally, a Blue Shifted Intermediate (BSI, λ_max = 498 nm, 100 K) is observed after the formation of E181Q Bathorhodopsin (Batho, λ_max = 556 nm, 10 K) but prior to formation of E181Q Lumirhodopsin (Lumi, λ_max = 506 nm, 220 K). A potential energy diagram of the observed photointermediates suggests the E181Q Batho intermediate has an enthalpy value 7.99 KJ/mol higher than E181Q BSI, whereas in rhodopsin, the BSI is 10.02 KJ/mol higher in enthalpy than Batho. Thus, the Batho to BSI transition is enthalpically driven in E181Q and entropically driven in native rhodopsin. We conclude that the substitution of Glu-181 with Gln-181 results in a significant perturbation of the hydrogen-bonding network within the active site of rhodopsin. In addition, the removal of a key electrostatic interaction between the chromophore and the protein destabilizes the protein in both the dark state and Batho intermediate conformations while having a stabilizing effect on the BSI conformation. The observed destabilization upon this substitution further supports that Glu-181 is negatively charged in the early intermediates of the photobleaching sequence of rhodopsin.

A methyl group at C7 of 11-cis-retinal allows chromophore formation but affects rhodopsin activation

The newly synthesized 11-cis-7-methylretinal can form an artificial visual pigment with kinetic and spectroscopic properties similar to the native pigment in the dark-state. However, its photobleaching behavior is altered, showing a Meta I-like photoproduct. This behavior reflects a steric constraint imposed by the 7-methyl group that affects the conformational change in the binding pocket as a result of retinal photoisomerization. Transducin activation is reduced, when compared to the native pigment with 11-cis-retinal. Molecular dynamics simulations suggest coupling of the C7 methyl group and the beta-ionone ring with Met207 in transmembrane helix 5 in agreement with recent experimental results.

Rhodopsin photointermediates in two-dimensional crystals at physiological temperatures

Bovine rhodopsin photointermediates formed in two-dimensional (2D) rhodopsin crystal suspensions were studied by measuring the time-dependent absorbance changes produced after excitation with 7 ns laser pulses at 15, 25, and 35 degrees C. The crystalline environment favored the Meta I(480) photointermediate, with its formation from Lumi beginning faster than it does in rhodopsin membrane suspensions at 35 degrees C and its decay to a 380 nm absorbing species being less complete than it is in the native membrane at all temperatures. Measurements performed at pH 5.5 in 2D crystals showed that the 380 nm absorbing product of Meta I(480) decay did not display the anomalous pH dependence characteristic of classical Meta II in the native disk membrane. Crystal suspensions bleached at 35 degrees C and quenched to 19 degrees C showed that a rapid equilibrium existed on the approximately 1 s time scale, which suggests that the unprotonated predecessor of Meta II in the native membrane environment (sometimes called MII(a)) forms in 2D rhodopsin crystals but that the non-Schiff base proton uptake completing classical Meta II formation is blocked there. Thus, the 380 nm absorbance arises from an on-pathway intermediate in GPCR activation and does not result from early Schiff base hydrolysis. Kinetic modeling of the time-resolved absorbance data of the 2D crystals was generally consistent with such a mechanism, but details of kinetic spectral changes and the fact that the residuals of exponential fits were not as good as are obtained for rhodopsin in the native membrane suggested the photoexcited samples were heterogeneous. Variable fractional bleach due to the random orientation of linearly dichroic crystals relative to the linearly polarized laser was explored as a cause of heterogeneity but was found unlikely to fully account for it. The fact that the 380 nm product of photoexcitation of rhodopsin 2D crystals is on the physiological pathway of receptor activation suggests that determination of its structure would be of interest.

Biochemical and physiological properties of rhodopsin regenerated with 11-cis-6-ring- and 7-ring-retinals

Phototransduction is initiated by the photoisomerization of rhodopsin (Rho) chromophore 11-cis-retinylidene to all-trans-retinylidene. Here, using Rho regenerated with retinal analogs with different ring sizes, which prevent isomerization around the C(11)=C(12) double bond, the activation mechanism of this G-protein-coupled receptor was investigated. We demonstrate that 11-cis-7-ring-Rho does not activate G-protein in vivo and in vitro, and that it does not isomerize along other double bonds, suggesting that it fits tightly into the binding site of opsin. In contrast, bleaching 11-cis-6-ring-Rho modestly activates phototransduction in vivo and at low pH in vitro. These results reveal that partial activation is caused by isomerization along other double bonds in more rigid 6-locked retinal isomers and protonation of key residues by lowering pH in 11-cis-6-ring-Rhos. Full activation is not achieved, because isomerization does not induce a complete set of conformational rearrangements of Rho. These results with 6- and 7-ring-constrained retinoids provide new insights into Rho activation and suggest a potential use of locked retinals, particularly 11-cis-7-ring-retinal, to inactivate opsin in some retinal degeneration diseases.

Bleaching kinetics of artificial visual pigments with modifications near the ring-polyene chain connection

Absorbance difference spectra were recorded at 20 degrees C from 30 ns to milliseconds after photolysis of lauryl maltoside suspensions of artificial visual pigments derived from 9-cis isomers of 5-ethylretinal, 8,16-methanoretinal (a 6-s-trans-bicyclic analogue), or 5-demethyl-8-methylretinal. In all three pigments, the earliest intermediate that was detected had the characteristics of a mixture of bathorhodopsin and a blue-shifted intermediate, BSI, which is the first decay product of bathorhodopsin in bovine rhodopsin. The first decays resolved on the nanosecond time scale were the formation of the lumirhodopsin analogues. Subsequent decays were able to be fit with a mechanistic scheme which has been shown to apply to both membrane and detergent suspensions of rhodopsin. Large increases were seen in the amount of metarhodopsin I which appeared after photolysis of 5-ethylisorhodopsin and the bicyclic isorhodopsin analogue, while 5-demethyl-8-methylisorhodopsin more closely followed native rhodopsin in decaying through meta I380, a 380 nm absorbing precursor to metarhodopsin II. In addition to forming more metarhodopsin I, the bicyclic analogue stabilized the metarhodopsin I-metarhodopsin II equilibrium similarly to what has been previously reported for 9-demethylrhodopsin in detergent, introducing the possibility that the bicyclic analogue could similarly be defective in transducin activation. These observations support the idea that long after initial photolysis, structural details of the retinylidene chromophore continue to play a decisive role in processes leading to the activated form, metarhodopsin II.

Steric barrier to bathorhodopsin decay in 5-demethyl and mesityl analogues of rhodopsin

Absorbance difference spectra were recorded from 20 ns to 1 micros after 20 degrees C photoexcitation of artificial visual pigments derived either from 5-demethylretinal or from a mesityl analogue of retinal. Both pigments produced an early photointermediate similar to bovine bathorhodopsin (Batho). In both cases the Batho analogue decayed to a lumirhodopsin (Lumi) analogue via a blue-shifted intermediate, BSI, which formed an equilibrium with the Batho analogue. The stability of 5-demethyl Batho, even though the C8-hydrogen of the polyene chain cannot interact with a ring C5-methyl group to provide a barrier to Batho decay, raises the possibility that the 5-demethylretinal ring binds oppositely from normal to form a pigment with a 6-s-trans ring-chain conformation. If 6-s-trans binding occurred, the ring C1-methyls could replace the C5-methyl in its interaction with the chain C8-hydrogen to preserve the steric barrier to Batho decay, consistent with the kinetic results. The possibility of 6-s-trans binding for 5-demethylretinal also could account for the unexpected blue shift of 5-demethyl visual pigments and could explain why 5-demethyl artificial pigments regenerate so slowly. Although the mesityl analogue BSI's absorption spectrum was blue-shifted relative to its pigment spectrum, the blue shift was much smaller than for rhodopsin's or 5-demethylisorhodopsin's BSI. This suggests that increased C6-C7 torsion may be responsible for some of BSI's blue shift, which is not the case for mesityl analogue BSI either because of reduced spectral sensitivity to C6-C7 torsion or because the symmetry of the mesityl retinal analogue precludes having 6-s-cis and 6-s-trans conformers. The similarity of the mesityl analogue BSI and native BSI lambda(max) values supports the idea that BSI has a 6-s angle near 90 degrees, a condition which could disconnect the chain (and BSI's spectrum) from the double bond specifics of the ring.

Movement of retinal along the visual transduction path

Movement of the ligand/receptor complex in rhodopsin (Rh) has been traced. Bleaching of diazoketo rhodopsin (DK-Rh) containing 11-cis-3-diazo-4-oxo-retinal yields batho-, lumi-, meta-I-, and meta-II-Rh intermediates corresponding to those of native Rh but at lower temperatures. Photoaffinity labeling of DK-Rh and these bleaching intermediates shows that the ionone ring cross-links to tryptophan-265 on helix F in DK-Rh and batho-Rh, and to alanine-169 on helix D in lumi-, meta-I-, and meta-II-Rh intermediates. It is likely that these movements involving a flip-over of the chromophoric ring trigger changes in cytoplasmic membrane loops resulting in heterotrimeric guanine nucleotide-binding protein (G protein) activation.

Effects of pH on rhodopsin photointermediates from lumirhodopsin to metarhodopsin II

Time-resolved absorption difference spectra of membrane suspensions of bovine rhodopsin at pH 5, 6, 7, 8, 9, and 10 were collected in the time range from 1 micro s to 200 ms after laser photolysis with 7-ns pulses of 477-nm light. The data were analyzed using singular value decomposition (SVD) and global exponential fitting. At pH 7 the data agree well with previously obtained data (Thorgeirsson et al. (1993) Biochemistry 32, 13861-13872) with fits improved at all pH's by inclusion of a small component due to an absorbance change caused by rotational diffusion which is detectable even at magic angle polarization. A "square scheme" suggested to best explain the previous data, which involves two branches following decay of the lumi intermediate with pathways (1) lumi --> MI480 right harpoon over left harpoon MII and (2) lumi right harpoon over left harpoon MI380 --> MII, could be confirmed throughout the entire pH range. However, to account for the increased rate of the MII --> MI480 reaction in path 1 for rising pH values, we propose that the MII in the square scheme consists of deprotonated MII and protonated MIIH+ forms in rapid equilibrium with each other, resulting in an extended square scheme and increasing the number of 380-nm products from two to three. In addition to the kinetic processes described by the extended square scheme, above pH 8 fast ( approximately 10 micro s) and slow ( approximately 50 ms) components were found. The fast component was assigned to the decay of a blue-shifted lumi intermediate, and the slow component, resolvable only at pH 10, was assigned to formation of a 450 nm absorbing photoproduct.

Presence of two rhodopsin intermediates responsible for transducin activation

To identify how many rhodopsin intermediates interact with retinal G-protein transducin, the photobleaching process of chicken rhodopsin has been investigated in the presence or absence of transducin by means of time-resolved low-temperature spectroscopy. Singular value decomposition (SVD) analysis of the spectral data showed that a new intermediate called meta Ib is present between formally identified metarhodopsin I (now referred to as meta Ia) and metarhodopsin II (meta II). Since the absorption maximum of meta Ib (460 nm) is similar to that of meta Ia (480 nm), but considerably different from that of meta II (380 nm), meta Ib should have a protonated retinylidene Schiff base as its chromophore. Whereas transducin showed no effect on the conversion process between lumirhodopsin (lumi) and meta Ia, it affected the process between meta Ia and meta Ib and that between meta Ib and meta II. These results suggest that at least two intermediates (meta Ib and meta II) interact with transducin. The addition of GTPgammaS had no effect on the meta Ib-transducin interaction, while it abolished the ability of transducin to interact with meta II. Thus, meta Ib only binds to transducin, while meta II catalyzes a GDP-GTP exchange in transducin. These results suggest that deprotonation of the Schiff base chromophore is not necessary for the binding to transducin, while changes in protein structure including Schiff base deprotonation are needed to induce the GDP-GTP exchange in transducin.

Properties of early photolysis intermediates of rhodopsin are affected by glycine 121 and phenylalanine 261

Glycine 121 in transmembrane (TM) helix 3 and phenylalanine 261 in TM helix 6 of bovine rhodopsin have been shown to be critical residues for creating an appropriate chromophore binding pocket for 11-cis-retinal [Han, M., Lin, S. W., Smith, S. O., and Sakmar, T. P. (1996) J. Biol. Chem. 271, 32330-32336; Han, M., Lin, S. W., Minkova, M., Smith, S. O., and Sakmar, T. P. (1996) J. Biol. Chem. 271, 32337-32342]. To further explore structure-function relationships in the vicinity of receptor helices 3 and 6, time-resolved absorption difference spectra of rhodopsin mutants G121A, G121V, and G121L/F261A were obtained at 20 degrees C. Data were collected from 30 ns to 690 ms after laser photolysis with 7 ns pulses (lambdamax = 477 nm) and analyzed using a global exponential fitting procedure after singular value decomposition (SVD). For each mutant, the decay of its bathorhodopsin photoproduct (batho) into an equilibrium with its blue-shifted intermediate (bsi) was too fast to resolve (<20 ns). The reaction scheme found for the mutants G121A and G121L/F261A was batho/bsi --> lumirhodopsin (lumi) --> metarhodopsin I (MI) --> metarhodopsin II (MII). For G121V, an additional early 380 nm absorber, with a back-reaction to lumi, had to be included in the above scheme. For the three Gly121 mutants, the main pathway to reach the active MII state is via lumi and MI. This is in contrast to rhodopsin where the main pathway in detergent samples is via lumi and an early 380 nm absorber, MI380. From the accelerated batho decay present in all three mutants, we conclude that Gly121 is likely to participate in the earliest chromophore-protein interactions. In addition, bsi decay is further accelerated in mutant G121L/F261A, suggesting that Phe261 is an essential determinant of the protein processes involved in bsi decay.

Chromophore structural changes in rhodopsin from nanoseconds to microseconds following pigment photolysis

Rhodopsin is a prototypical G protein-coupled receptor that is activated by photoisomerization of its 11-cis-retinal chromophore. Mutant forms of rhodopsin were prepared in which the carboxylic acid counterion was moved relative to the positively charged chromophore Schiff base. Nanosecond time-resolved laser photolysis measurements of wild-type recombinant rhodopsin and two mutant pigments then were used to determine reaction schemes and spectra of their early photolysis intermediates. These results, together with linear dichroism data, yielded detailed structural information concerning chromophore movements during the first microsecond after photolysis. These chromophore structural changes provide a basis for understanding the relative movement of rhodopsin's transmembrane helices 3 and 6 required for activation of rhodopsin. Thus, early structural changes following isomerization of retinal are linked to the activation of this G protein-coupled receptor. Such rapid structural changes lie at the heart of the pharmacologically important signal transduction mechanisms in a large variety of receptors, which use extrinsic activators, but are impossible to study in receptors using diffusible agonist ligands.

Time-resolved spectroscopy of the early photolysis intermediates of rhodopsin Schiff base counterion mutants

Time-resolved absorption difference spectra of COS-cell expressed rhodopsin and rhodopsin mutants (E113D, E113A/A117E, and G90D), solubilized in detergent, were collected from 20 ns to 510 ms after laser photolysis with 7 ns pulses (lambda(max) = 477 nm). The data were analyzed using a global exponential fitting procedure following singular value decomposition (SVD). Over the entire time range excellent agreement was achieved between results for COS-cell and rod outer segment rhodopsin both in kinetics and in the lambda(max) values of the intermediates. The Schiff base counterion mutant E113D showed strong similarities to rhodopsin up to lumi, following the established scheme: batho <==> bsi --> lumi. Including late delay times (past 1 micros), the mutant E113D lumi decayed to metarhodopsin II (MII), showing that the detergent strongly favors MII over metarhodopsin I (MI). However, a back-reaction from MII to lumi was observed that was not seen for rhodopsin. The kinetic schemes for the mutants E113A/A117E and G90D were significantly different from that of rhodopsin. In both mutants batho decay into an equilibrium with bsi was too fast to resolve (<20 ns). The batho/bsi mixtures decayed with the following reaction scheme: batho/bsi <==> lumi <==> MI-like <==> MII-like. However, the back-reaction from MI-like to lumi was not seen in G90D. MI-like spectral intermediates absorbing around 460 nm appeared in both mutants. They have been shown to be the transducin-activating species (R*). These data, interpreted in the context of previous NMR, FTIR, and Raman data, are consistent with a picture in which the kinetics of batho decay is dependent on a protein-induced perturbation near C12-C13 of the retinal chromophore. The lambda(max) values of the bsi and lumi intermediates in the mutant pigments are interpreted in terms of movement of the Schiff base relative to its counterion.

Chromophore configuration of iodopsin and its photoproducts formed at low temperatures

The photochemical reactions of iodopsin at low temperatures were investigated by a combination of absorption spectroscopy and chromophore extraction to show the formation of isomeric photoproducts other than the all-trans intermediates. We first confirmed that the chromophore in iodopsin is an 11-cis-retinal. Next, iodopsin samples were irradiated with light of different wavelengths at selected temperatures ranging from -190 to 0 degrees C, and their retinylidene chromophores were extracted as oximes after warming the sample to 0 degree C. The isomeric composition of the extracted chromophores was analyzed by high-performance liquid chromatography. It was confirmed that bathoiodopsin produced at -190 degrees C has an all-trans chromophore, but a considerable amount of its chromophore thermally reisomerizes to the 11-cis form upon warming. Photoproducts formerly assigned as lumi- and metaiodopsins [Yoshizawa, T., & Wald, G. (1967) Nature 214, 566-571; Hubbard, R., & Kropf, A. (1959) Nature 183, 448-450] were produced by extensive irradiation of iodopsin at -80 and -40 degrees C, respectively, with red light, but their chromophores were identified to be 7-cis-retinals instead of all-trans-retinals. Thus these photoproducts are artificial byproducts formed as a result of photon absorption by all-trans intermediates. The absorption spectrum of the 7-cis product formed from bovine rhodopsin shows no spectral shift when it is warmed from -80 to 0 degrees C, but the spectrum of 7-cis species formed from iodopsin shifted about 40 nm to the blue at a transition temperature of -60 degrees C. This result indicates a unique chromophore-opsin interaction in iodopsin. Four all-trans intermediates of iodopsin were identified above -80 degrees C under irradiation conditions in which no 7-cis products accumulated. Their absorption maxima were estimated to be approximately 570, approximately 530, approximately 470, and approximately 380 nm. These species should correspond to BL-iodopsin, lumiiodopsin, metaiodopsin I, and metaiodopsin II, respectively, assigned by room temperature laser photolysis [Shichida, Y., Okada, T., Kandori, H., Fukada, Y., & Yoshizawa, T. (1993) Biochemistry 32, 10832-10838].

Structure around C6-C7 bond of the chromophore in bathorhodopsin: low-temperature spectroscopy of 6s-cis-locked bicyclic rhodopsin analogs

To elucidate the structural changes near the beta-ionone ring region of the chromophore during the photobleaching process of rhodopsin, the photochemical and subsequent thermal reactions of rhodopsin analogs, whose retinylidene chromophores were fixed in a 6s-cis form with a five-membered ring (6,5-rhodopsin) and a seven-membered ring (6,7-rhodopsin), respectively, were investigated by low-temperature spectroscopy. Like rhodopsin, both the rhodopsin analogs convert to the respective batho-intermediates upon absorption of light at -190 degrees C. The extinction coefficient of batho-intermediate of 6,5-rhodopsin is similar to that of bathorhodopsin, while that of 6,7-rhodopsin is considerably smaller than that of bathorhodopsin. Like bathorhodopsin, the batho-intermediate of 6,5-rhodopsin directly converts to lumi-intermediate, while that of 6,7-rhodopsin first converts to a blue-shifted intermediate and then to lumi-intermediate. These results strongly suggest that the structure around the beta-ionone ring region of the bathorhodopsin chromophore resembles 6,5-retinal rather than 6,7-retinal. From the comparison of the structural features among retinal, 6,5-retinal, and 6,7-retinal, a possible conformation around C6-C7 bond of the bathorhodopsin chromophore is discussed.

Low-temperature trapping of early photointermediates of alpha-isorhodopsin

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

Direct observation of the thermal equilibria among lumirhodopsin, metarhodopsin I, and metarhodopsin II in chicken rhodopsin

Using low-temperature time-resolved spectroscopy, we have directly observed thermal back reaction of metarhodopsin I (meta I) to lumirhodopsin (lumi) and that of metarhodopsin II (meta II) to meta I in chicken rhodopsin to demonstrate the presence of thermal equilibria among lumi, meta I, and meta II. The back reaction from meta I to lumi was observed when the rhodopsin sample irradiated at -35 degrees C was warmed to -20 degrees C, while that from meta II to meta I was observed when the sample irradiated at -10 degrees C was cooled to -20 degrees C. Thermodynamic parameters of lumi, meta I, and meta II were calculated from the equilibrium constants estimated by analyzing the spectra of the equilibrium states at temperatures ranging from -30 to -10 degrees C. The results showed that meta I has an enthalpy and an entropy considerably smaller than those of lumi and meta II, while the difference in thermodynamic parameters between lumi and meta II is not so large. These results suggest that meta I is a crucial stage of conversion of the light energy captured by the chromophore into restricted conformations of the chromophore and/or protein, from which a large conformational change of the protein starts to form meta II.

Effects of temperature on rhodopsin photointermediates from lumirhodopsin to metarhodopsin II

Absorbance changes following the photolysis of mildly sonicated membrane suspensions of bovine rhodopsin are monitored using multichannel detection at 15, 20, 25, 30, and 35 degrees C. Difference spectra collected with microsecond time resolution are analyzed by singular value decomposition and multiexponential fitting. Several kinetic schemes are tested using methods that compare the observed rates and associated spectral amplitudes to the eigenvalues and eigenvectors of kinetic matrices. The time evolution of the spectra is more complex than can be accounted for by the traditional lumi-->metarhodopsin I<-->metarhodopsin II scheme. Above 25 degrees C, the formation of metarhodopsin II is achieved without a large transient accumulation of metarhodopsin I. Within the framework of first-order kinetics, the observations are explained by simple kinetic schemes that lead to the formation of a deprotonated Schiff's base species temporally distinct from metarhodopsin II directly upon the decay of lumirhodopsin.

pKa of the protonated Schiff base of bovine rhodopsin. A study with artificial pigments

Artificial bovine rhodopsin pigments derived from synthetic retinal analogues carrying electron-withdrawing substituents (fluorine and chlorine) were prepared. The effects of the electron withdrawing substituents on the pKa values of the pigments and on the corresponding Schiff bases in solution were analyzed. The data suggest that the apparent pKa of the protonated Schiff base is above 16. However, the alternative possibility that the retinal Schiff base linkage in bovine rhodopsin is not accessible for titration from the aqueous bulk medium cannot be definitely ruled out.

Photolysis of rhodopsin results in deprotonation of its retinal Schiff's base prior to formation of metarhodopsin II

Absorption changes following photolysis of bovine rhodopsin in mildly sonicated membrane suspensions are monitored at 25 degrees C. Difference spectra collected at 17 times between 1 microsecond and 75 ms following excitation are analyzed globally using singular value decomposition and non-linear least-squares fitting techniques. The results are not consistent with the simple scheme: Lumirhodopsin-->Metarhodopsin I<-->Metarhodopsin II, but indicate that an intermediate with a deprotonated Schiff's base is formed nearly simultaneously with metarhodopsin I upon the decay of Lumirhodopsin.

Photointermediates of visual pigments

Much progress has been made in recent years toward understanding the interactions between various proteins responsible for visual transduction which are initiated by an activated state of visual pigments. However, the changes which take place in the visual pigments themselves to convert them to the activated state are more poorly understood. Many spectroscopic techniques have been applied to this problem in recent years and considerable progress has been made. A major goal of these efforts is to understand at which stages protein change occurs and to characterize its structural features. In the visual system evidence is accumulating, for example, that chromophore independent protein change begins immediately prior to lumirhodopsin formation. Considerable insight has been gained recently into the early intermediates of visual transduction and the stage is set to achieve similar understanding of the later intermediates leading to rhodopsin's activated state.

Early photolysis intermediates of the artificial visual pigment 13-demethylrhodopsin

Nanosecond time-resolved absorption measurements are reported for the room temperature photolysis of a modified rhodopsin pigment, 13-demethylrhodopsin, which contains the chromophore 13-demethylretinal. The measurements are consistent with the formation of an equilibrium between a BA-THO-13-demethylrhodopsin species and a blue-shifted species (relative to the parent pigment), BSI-13-demethylrhodopsin. The results are compared to those acquired after photolysis of native bovine rhodopsin [Hug, S. J., Lewis, J. W., Einterz, C. M., Thorgeirsson, T. E., & Kliger, D. S. (1990) Biochemistry (preceding paper in this issue)] and to results obtained after photolysis of several modified isorhodopsin pigments in which the BSI species was first observed. It is concluded that in all of the pigments the results are consistent with the formation of an equilibrium between BATHO and BSI, which subsequently decays on a nanosecond time scale at room temperature to a lumirhodopsin intermediate.

Transition dipole orientations in the early photolysis intermediates of rhodopsin

The linear dichroism spectrum of rhodopsin in sonicated bovine disk membranes was measured 30, 60, 170, and 600 ns after room temperature photolysis with a linearly polarized, 7-ns laser pulse (lambda = 355 or 477 nm). A global exponential fitting procedure based on singular value decomposition was used to fit the linear dichroism data to two exponential processes which differed spectrally from one another and whose lifetimes were 42 +/- 7 ns and 225 +/- 40 ns. These results are interpreted in terms of a sequential model where bathorhodopsin (BATHO, lambda max = 543 nm) decays toward equilibrium with a blue shifted intermediate (BSI, lambda max = 478 nm). BSI then decays to lumirhodopsin (LUMI, lambda max = 492 nm). It has been suggested that two bathorhodopsins decay in parallel to their products. However, a Monte Carlo simulation of partial photolysis of solid-state visual pigment samples shows that one mechanism which creates populations of BATHO having different photolysis rates at 77 K may not be responsible for the two decay rates reported here at room temperature. The angle between the cis band and 498-nm band transition dipoles of rhodopsin is determined to be 38 degrees. The angles between both these transition dipoles and those of the long-wave-length bands of BATHO, BSI, and LUMI are also determined. It is shown that when BATHO is formed its transition dipole moves away from the original cis band transition dipole direction. The transition dipole then moves roughly twice as much towards the original cis band direction when BSI appears. Production of LUMI is associated with return of the transition dipole almost to the original orientation relative to the cis band, but with some displacement normal to the plane which contains the previous motions. The correlation between the lambda max of an intermediate and its transition dipole direction is discussed.