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Investigation of the proton release channel of bacteriorhodopsin in different intermediates of the photo cycle. A molecular dynamics study.

Molecular dynamics simulations on bacteriorhodopsin were performed starting from a conformation based on electron cryomicroscopy studies [Henderson, R., et al. (1990) J. Mol. Biol. 213, 899-929]. We examined the proton release channel in different intermediates of the bacteriorhodopsin photocycle. In the simulations of the ground state, two stable sets of conformations were observed differing in the distance of the guanidinium group of Arg82 to the Schiff base. The set of conformations in which Arg82 is located closer to the Schiff base has a lower potential energy and agrees better with experimental data than the other set. With both sets, we performed a series of simulations in which the chromophore was isomerized to different states using purposive and nonpurposive methods. The energetic consideration of the different states argues for the location of the guanidinium group of Arg82 close to the Schiff base. The results also show that no C13-C14, C14-C15 dicis conformation of the retinal occurs in the K/L-intermediate of the photocycle instead supporting the occurrence of C13-C14 cis in these intermediates. In a last series of simulations, we modeled the M-intermediate of the bacteriorhodopsin photocycle. Again, comparison to different experimental data indicates that Arg82 points toward the Schiff base. We conclude that the guanidinium group of Arg82 is located close to the Schiff base at a distance of approximately 4.5 A and stays there at least up to the M-intermediate of the photocycle.

Arginine↗

Trp86 --> Phe replacement in bacteriorhodopsin affects a water molecule near Asp85 and light adaptation.

Illumination of the Trp86 --> Phe mutant of bacteriorhodopsin causes anomalous light adaptation, i.e., isomerization of the retinal from all-trans to 13-cis, 15-syn. FTIR spectral analysis shows that illumination at 250 K yields two 13-cis photoproducts, the conventional 13-cis, 15-syn state, BR(C), and another termed BR(X). BR(X) is different from BR(C) because it has a lower N-H in-plane bending frequency and a higher C14-C15 stretching frequency, as well as an absence of coupling between these modes. BR(X), which is stable at 275 K, is more abundant in the photosteady state produced by longer wavelength light and detected as the only photoproduct at 170 K. Its different structural features result from distortion of the C14-C15 bond of the chromophore. In the W86F mutant protein, the small structural changes of a water molecule in the conversion between the all-trans and 13-cis, 15-syn forms and in the formation of the K photointermediate are absent, but the larger changes of water molecule(s) that normally occur in the L and M intermediates are present. We propose that Trp86, together with Asp85, is involved in binding the water molecule and in preventing the formation of the 13-cis, 15-syn photoproducts, BR(C) and BR(X), when the wild type protein is illuminated.

Aspartic Acid↗

Early photolysis intermediates of gecko and bovine artificial visual pigments.

Nanosecond laser photolysis measurements were conducted on digitonin extracts of artificial pigments prepared from the cone-type visual pigment, P521, of the Tokay gecko (Gekko gekko) retina. Artificial pigments were prepared by regeneration of bleached gecko photoreceptor membranes with 9-cis-retinal, 9-cis-14-methylretinal, or 9-cis-alpha-retinal. Absorbance difference spectra were recorded at a sequence of time delays from 30 ns to 60 microseconds following excitation with a pulse of 477-nm actinic light. Global analysis showed the kinetic data for all three artificial gecko pigments to be best fit by two-exponential processes. These two-exponential decays correspond to similar decays observed after photolysis of P521 itself, with the first process being the decay of the equilibrated P521 Batho<-->P521 BSI mixture to P521 Lumi and the second process being the decay of P521 Lumi to P521 Meta I. In spite of its large blue shift relative to P521, iso-P521 displays a normal chloride depletion induced blue shift. Iso-P521's early intermediates up to Lumi were also blue-shifted, with the P521 Batho<-->P521 BSI equilibrated mixture being 15 nm blue-shifted and P521 Lumi being 8 nm blue-shifted relative to the intermediates formed after P521 photolysis. The blue shift associated with the iso-pigment is reduced or disappears entirely by P521 Meta I. Similar blue shifts were observed for the early intermediates observed after photolysis of bovine isorhodopsin, with the Lumi intermediate blue-shifted 5 nm compared to the Lumi intermediate formed after photolysis of bovine rhodopsin. These shifts indicate that a difference exists between the binding sites of 9- and 11-cis pigments which persists for microseconds at 20 degrees C.

Animals↗

Ultraviolet resonance Raman spectra of Trp-182 and Trp-189 in bacteriorhodopsin: novel information on the structure of Trp-182 and its steric interaction with retinal.

Ultraviolet (244 nm) resonance Raman spectra of Trp-182 and Trp-189 in bacteriorhodopsin were obtained by subtracting the spectrum of the mutants, Trp-182-->Phe or Trp-189-->Phe, from that of the wild-type. Analysis of the spectra shows that the chi2,1 torsion angle about the Cbeta-C3 bond is +/-93 degrees for Trp-182 and +/-100 degrees for Trp-189. Both Trp residues are moderately hydrogen bonded to proton acceptors at their indolyl nitrogens in hydrophobic environments. The environmental hydrophobicity is particularly strong for Trp-182, as judged from the splitting of the W7 Raman band to a triplet. The Raman information on the structure and environment of Trp-189 is consistent with the molecular model from electron diffraction [Grigorieff et al. (1996) J. Mol. Biol. 259, 393-421]. On the other hand, the chi2,1 angle and the hydrogen-bonding state of Trp-182 found here differ from those in the model structure. Revision of the model to correspond to the Raman findings would require a 60 degrees rotation of the Trp-182 indole ring about the Cbeta-C3 bond toward the chromophore retinal and the presence of a water molecule that is hydrogen bonded to the indolyl nitrogen. The triplet feature of the W7 band of Trp-182 is attributable to unusually strong steric repulsion between the indole ring and the 9- and 13-methyl groups of the retinal. Resonance Raman spectra in the visible suggest that this steric conflict destabilizes the 13-cis isomeric state of the retinal.

Bacteriorhodopsins↗

Free-energy simulations of the retinal cis --> trans isomerization in bacteriorhodopsin.

Free-energy profiles for ground-state cis --> trans isomerization of retinal in vacuum, in solution, and in the protein bacteriorhodopsin are calculated using free-energy simulations. The free-energy barriers in the protein were 9 kcal/mol for ionized Asp85 and 14 kcal/mol for neutral Asp85, significantly lower than those found in solution (18 kcal/mol) or vacuum (19 kcal/mol). Therefore, bacteriorhodopsin can be said to act as a catalyst in the isomerization. The barrier in the protein is due mainly to stabilization of the transition state through favorable nonbonded interactions with the protein part of the system, with internal strain and interactions with solvent playing minor roles. The protonated Asp85 simulation models the behavior of the system in the N --> O transition. Our calculated 14 kcal/mol barrier and 4-ms relaxation time for this process are in excellent agreement with experimentally measured values of 12 kcal/mol and 5 ms, respectively. The ionized Asp85 simulation models two hypothetical processes: the N --> O transition with a proton removed from Asp85 and the initial BR568 --> L transition on the ground-state energy surface. The cis-trans isomerization barrier in this system is 9 kcal/mol, the lowest of all the studied cases. The presence of the charged carboxylate group in the ionized Asp85 system leads to strong stabilization of the transition state by interactions with the surroundings and changes the distance between Asp85 and the Schiff base proton compared to the corresponding distance in the neutral Asp85 system. This suggests that the protonation of Asp85 plays an important role in regulating access to the Schiff base proton. For both Asp85 ionization states the calculated cis-trans free-energy difference was close to 0, indicating that the protein can accommodate both retinal isomers equally well. The computed negligible difference between the N and O free-energy levels is in accord with experimental data.

Bacteriorhodopsins↗

Existence of a proton transfer chain in bacteriorhodopsin: participation of Glu-194 in the release of protons to the extracellular surface.

Glu-194 near the extracellular surface of bacteriorhodopsin is indispensable for proton release to the medium upon protonation of Asp-85 during light-driven transport. As for Glu-204, its replacement with glutamine (but not aspartate) abolishes both proton release and the anomalous titration of Asp-85 that originates from coupling between the pKa of this buried aspartate and those of the other acidic groups. Unlike the case of Glu-204, however, replacement of Glu-194 with aspartate raises the pKa for proton release. In Fourier transform infrared spectra of the E194D mutant a prominent positive band is observed at 1720 cm-1. It can be assigned from [4-13C]aspartate and D2O isotope shifts to the C&dbd;O stretch of protonated Asp-194. Its rise correlates with proton transfer from the retinal Schiff base to Asp-85. Its decay coincides with the appearance of a proton at the surface, detected under similar conditions with fluorescein covalently bound to Lys-129 and with pyranine. Its amplitude decreases with increasing pH, with a pKa of about 9. We show that this pKa is likely to be that of the internal proton donor to Asp-194, the Glu-204 site, before photoexcitation, while 13C NMR titration indicates that Asp-194 has an initial pKa of about 3. We propose that there is a chain of interacting residues between the retinal Schiff base and the extracellular surface. After photoisomerization of the retinal the pKa's change so as to allow (i) Asp-85 to become protonated by the Schiff base, (ii) the Glu-204 site to transfer its proton to Asp-194 in E194D, and therefore to Glu-194 in the wild type, and (iii) residue 194 to release the proton to the medium.

Bacteriorhodopsins↗

Role of the C9 methyl group in rhodopsin activation: characterization of mutant opsins with the artificial chromophore 11-cis-9-demethylretinal.

Activation of the visual pigment rhodopsin involves both steric and electrostatic interactions between the chromophore and opsin within the retinal-binding site. Removal of the C9 methyl group of 11-cis-retinal inhibits light-dependent activation of the G protein, transducin, suggesting a direct steric contact. More recently, we have shown that steric interactions lead to receptor activation when Gly121 in the middle of transmembrane helix 3 is replaced by larger hydrophobic residues. In order to understand in more detail the role of the C9 methyl group of retinal in the structure and function of rhodopsin, we first studied the properties of recombinant 9-dm-Rho (opsin reconstituted with 11-cis-9-demethylretinal). The 9-dm-Rho pigment displayed a blue-shifted lambdamax, increased hydroxylamine reactivity, and decreased ability to activate transducin. These properties are consistent with the hypothesis that the C9 methyl group is a crucial structural anchor for the correct docking of the chromophore in its binding site. Next, we investigated the possible interaction between Gly121 of opsin and the C9 methyl group of retinal by characterizing recombinant pigments produced by combining mutant opsins (G121A, -V, -I, -L, and -W) with 11-cis-9-demethylretinal. Mutant opsins G121I, -L, and -W failed to bind the chromophore. However, the double mutant G121L/F261A bound 11-cis-9-demethylretinal to form a stable pigment with a lambdamax of 451 nm. When activity was assayed in membranes, the reduction in transducin activation by 9-dm-Rho caused by the lack of a C9 methyl group on the chromophore could be partially restored by replacing Gly121 with a bulky residue (leucine, isoleucine, or tryptophan). These results support a model of receptor activation that involves steric interaction between the C9 methyl group of the chromophore and the opsin in the vicinity of Gly121 on transmembrane helix 3.

Isomerism↗

An additional methyl group at the 10-position of retinal dramatically slows down the kinetics of the rhodopsin photocascade.

The present study focuses on ligand-protein interactions in a rhodopsin analogue generated from bovine opsin and the 10-methyl homologue of 11-cis-retinal. The analogue pigment displays a reduced alpha-band at 506 +/- 2 and a stronger beta-band at 325 nm. Remarkably, the rotational strength of these bands observed in visible circular dichroism spectra was found to be similar for both native and 10-methyl rhodopsin. The quantum yield of the analogue pigment was determined to be 0.55. All photointermediates were analyzed by Fourier transform infrared difference spectroscopy. At the batho stage, strong hydrogen-out-of-plane vibrations were observed, indicating that the 10-methyl chromophore also adopts a distorted all-trans conformation at this stage. In contrast to native rhodopsin, the batho intermediate of the 10-methyl pigment is stable up to 180 K and only slowly decays to the next intermediate between 180 and 210 K. As in native rhodopsin, the 10-methyl metarhodopsin I intermediate is generated at about 220 K, but its transition to the metarhodopsin II state is again shifted to a much higher temperature (> 293 K) than for the native pigment (> 260 K). Infrared analysis, nevertheless, shows that the conformational changes in the photointermediates of the 10-methyl pigment are basically identical with those observed in the native pigment. This is supported by a signal function assay, showing that the analogue pigment is able to activate transducin. The dual effect of the 10-methyl group on the photocascade is attributed to steric interactions which, initially, hamper the relaxation of strain in the polyene chain of the chromophore and, eventually, interfere with the conformational rearrangements of the protein moiety required to adopt the active conformation of the receptor. Our data provide direct support for the concept that the relaxation of strain in the retinal polyene chain acts as the major driving force of the photocascade dark reaction.

Animals↗

Local-access model for proton transfer in bacteriorhodopsin.

The accessibility of the retinal Schiff base in bacteriorhodopsin was studied in the D85N/D96N mutant where the proton acceptor and donor are absent. Protonation and deprotonation of the Schiff base after pH jump without illumination and in the photocycle of the unprotonated Schiff base were measured in the visible and the infrared. Whether access is extracellular (EC) or cytoplasmic (CP) was decided from the effect of millimolar concentrations of azide on the rates of proton transfers. The results, together with earlier work on the wild-type protein, suggest a new hypothesis for the proton-transfer switch: (i) In the metastable 13-cis, 15-anti and all-trans, 15-syn photoproducts, but not in the stable isomeric states, access flickers between the EC and CP directions. (ii) The direction of proton transfer is decided both by this local access and by the presence of a suitable donor or acceptor group (in the wild type), or the proton conductivity in the EC and CP half-channels (in D85N/D96N). (iii) Thermal reisomerization of the retinal can occur only when the Schiff base is protonated, as is well-known. In the wild-type transport cycle, the concurrent local EC and CP access during the lifetime of the metastable 13-cis, 15-anti state enables the changing pKa's of the proton acceptor and donor to determine the direction of proton transfer. Proton transfer from the Schiff base to Asp-85 in the EC direction is followed by reprotonation by Asp-96 from the CP direction because proton release to the EC surface raises the pKa of Asp-85 and a large-scale protein conformation change lowers the pKa of Asp-96. The unexpected finding we report here for D85N/D96N, that when the retinal is in the stable all-trans, 15-anti and 13-cis, 15-syn isomeric forms access of the Schiff base is locked (in the EC and CP directions, respectively), suggests that in this protein reisomerization, rather than changes in the proton conductivities of the EC and CP half-channels, provides the switch function. With this mechanism, the various modes of transport reported for Asp-85 mutants (CP to EC direction with blue light, and EC to CP direction with blue plus green light) are understood also in terms of rules i-iii.

Amino Acid Substitution↗

Rhodopsin arginine-135 mutants are phosphorylated by rhodopsin kinase and bind arrestin in the absence of 11-cis-retinal.

Arginine-135, located at the border between the third transmembrane domain and the second cytoplasmic loop of rhodopsin, is one of the most highly conserved amino acids in the family of G protein-coupled receptors. The effect of mutation at Arg-135 on the ability of rhodopsin to undergo desensitization was investigated. Four mutants, R135K, R135Q, R135A, and R135L, were examined for their ability to be phosphorylated by rhodopsin kinase, to bind arrestin, and to activate the rod cell G protein, transducin (Gt). All of the mutants were phosphorylated, bound arrestin, and were able to activate Gt when reconstituted with 11-cis-retinal. Surprisingly, several of the mutants could be phosphorylated by rhodopsin kinase and could bind arrestin in the absence of 11-cis-retinal but were not able to activate Gt. These observations represent the first demonstration of a mutant G protein-coupled receptor that assumes a conformation able to interact with its G protein-coupled receptor kinase and arrestin, but not with its G protein, in the absence of ligand.

Animals↗

Conformational changes in the core structure of bacteriorhodopsin.

Bacteriorhodopsin (bR) is the light-driven proton pump found in the purple membrane of Halobacterium salinarium. In this work, structural changes occurring during the bR photocycle in the core structure of bR, which is normally inaccessible to hydrogen/deuterium (H/D) exchange, have been probed. FTIR difference bands due to vibrations of peptide groups in the core region of bR have been assigned by reconstituting and regenerating delipidated bR in the presence of D2O. Exposure of bR to D2O even after long periods causes only a partial shift of the amide II band due to peptide NH --> ND exchange only of peripheral peptide structure. However, the amide II band completely downshifts when reconstitution/regeneration of bR is performed in the presence of D2O, indicating that almost the entire core backbone structure of bR undergoes H/D exchange. Peripheral regions can then be reexchanged in H2O, leaving the core backbone region deuterated. Low-temperature FTIR difference spectra on these core-deuterated samples reveal that peptide groups in the core region respond to retinal isomerization as early as the K intermediate. By formation of the M intermediate, infrared differences in the amide I region are dominated by much larger structural changes occurring in the core structure. In the amide II region, difference bands appear upon K formation and increase upon M formation which are similar to those observed upon the cooling of bacteriorhodopsin. This work shows that retinal isomerization induces conformational changes in the bacteriorhodopsin core structure during the early photocycle which may involve an increase in the strength of intramolecular alpha-helical hydrogen bonds.

Amides↗

Chromophore orientation in bacteriorhodopsin determined from the angular dependence of deuterium nuclear magnetic resonance spectra of oriented purple membranes.

The orientation of prosthetic groups in membrane proteins is of considerable importance in understanding their functional role in energy conversion, signal transduction, and ion transport. In this work, the orientation of the retinylidene chromophore of bacteriorhodopsin (bR) was investigated using 2H NMR spectroscopy. Bacteriorhodopsin was regenerated with all-trans-retinal stereospecifically deuterated in one of the geminal methyl groups on C1 of the cyclohexene ring. A highly oriented sample, which is needed to obtain individual bond orientations from 2H NMR, was prepared by forming hydrated lamellar films of purple membranes on glass slides. A Monte Carlo method was developed to accurately simulate the 2H NMR line shape due to the distribution of bond angles and the orientational disorder of the membranes. The number of free parameters in the line shape simulation was reduced by independent measurements of the intrinsic line width (1.6 kHz from T2e experiments) and the effective quadrupolar coupling constant (38. 8-39.8 kHz from analysis of the line shape of a powder-type sample). The angle between the C1-(1R)-1-CD3 bond and the purple membrane normal was determined with high accuracy from the simultaneous analysis of a series of 2H NMR spectra recorded at different inclinations of the uniaxially oriented sample in the magnetic field at 20 and -50 degrees C. The value of 68.7 +/- 2.0 degrees in dark-adapted bR was used, together with the previously determined angle of the C5-CD3 bond, to calculate the possible orientations of the cyclohexene ring in the membrane. The solutions obtained from 2H NMR were then combined with additional constraints from linear dichroism and electron cryomicroscopy to obtain the allowed orientations of retinal in the noncentrosymmetric membrane structure. The combined data indicate that the methyl groups on the polyene chain point toward the cytoplasmic side of the membrane and the N-H bond of the Schiff base to the extracellular side, i.e., toward the side of proton release in the pump pathway.

Bacteriorhodopsins↗

Partitioning of free energy gain between the photoisomerized retinal and the protein in bacteriorhodopsin.

Photoisomerization of the all-trans-retinal of bacteriorhodopsin to 13-cis,15-anti initiates a sequence of thermal reactions in which relaxation of the polyene chain back to all-trans is coupled to various changes in the protein and the translocation of a proton across the membrane. We investigated the nature of this high-energy state in a genetically modified bacteriorhodopsin. When the electric charges of residues 85 and 96, the two aspartic acids critical for proton transport, are both changed to what they become after photoexcitation of the wild-type protein, i.e., neutral and anionic, respectively, the retinal assumes a thermally stable 13-cis,15-anti configuration. Thus, we have reversed cause and effect in the photocycle. It follows that when the 13-cis,15-anti isomeric state is produced by illumination, in the wild type it is unstable initially only because of conflicts with the retinal binding pocket. Later in the photocycle, the free energy gain is transferred from the chromophore to the protein. Before recovery of the initial state, it will come to be represented entirely by the free energy of the changed protonation states of aspartic acids 85 and 96.

Amino Acid Substitution↗

Holo-cellular retinol-binding protein: distinction of ligand-binding affinity from efficiency as substrate in retinal biosynthesis.

Microsomal enzymes that catalyze the first step in the biosynthesis of retinoic acid from retinal, retinol dehydrogenases (RDHs), access retinol bound to cellular retinol-binding protein (CRBP). This study tested the hypothesis that the RDHs interact with the region in CRBP designated as the "helical cap" by evaluating single site-directed mutations, namely, L29A, I32E, L35A, L35E, L35R, L36A, F57A, R58A, and R58E. UV analysis showed mutants had similar conformations of retinol in their binding pockets. Nevertheless, the mutants bound retinol with affinities 2-5-fold lower than wild type, except for L35 mutants, which had affinities similar to wild type. All mutants' holoforms had more relaxed conformations about their helical caps, judged by sensitivity to partial protease digestion. Mutants showed no significant differences in Km values, but two (L36A, R58A) had increased Vm values and L35 mutants had decreased Vm values. Overall, the data indicate that the residues tested contribute in varying degrees to CRBP rigidity, retinol binding, and RDH recognition/access to bound retinol. The extent of contributions can be distinguished for several residues. For example, L35 mutants had lower kcat values than wild-type CRBP; thus, L35 seems important for RDH access to retinol. F57, on the other hand, a suspected key residue in controlling retinol entrance/exit, does not make a singular contribution to retinol binding. These results suggest a role for the helical cap region as a locus for RDH interaction and as a portal for ligand access to CRBP, and show that the affinity (Kd) of CRBP for retinol alone does not determine the efficiency of holo-CRBP as substrate. These are the first experimental data of enzyme recognition by a specific exterior residue of CRBP (L35).

Alcohol Oxidoreductases↗

Solid state 15N NMR evidence for a complex Schiff base counterion in the visual G-protein-coupled receptor rhodopsin.

Using the baculovirus/Sf9 cell expression system, we have incorporated 99% 15N-enriched [alpha,epsilon-15N2]-L-lysine into the rod visual pigment rhodopsin. We have subsequently investigated the protonated Schiff base (pSB) linkage in the [alpha, epsilon-15N2]Lys-rhodopsin with cross-polarization magic angle spinning (CP/MAS) 15N NMR. The Schiff base (SB) 15N in [alpha, epsilon-15N2]Lys-rhodopsin resonates with an isotropic shift sigmaI of 155.9 ppm, relative to 5.6 M 15NH4Cl. This suggests that the SB in rhodopsin is protonated and stabilized by a complex counterion. The 15N shifts of retinal SBs correlate with the energy difference between the ground and excited states and the frequency of maximum visible absorbance, numax, associated with the pi-pi transition of the polyene chromophore. Experimental modeling of the relation between the numax and the size of the counterion with a set of pSBs provides strong evidence that the charged chromophore in rhodopsin is stabilized by a counterion with an estimated effective center-center distance (deff) between the counterion and the pSB of 0.43 +/- 0.01 nm. While selected prokaryotic proteins and complexes have been labeled before, this is the first time to our knowledge that a 15N-labeled eukaryotic membrane protein has been generated in sufficient amount for such NMR investigations.

Animals↗

Existence of two L photointermediates of halorhodopsin from Halobacterium salinarium, differing in their protein and water FTIR bands.

FTIR difference spectra were recorded for the photoreactions of halorhodopsin from Halobacterium salinarium at 170 and 250 K. Obvious differences at the two temperatures were noted in neither the visible spectra nor the FTIR bands of the chromophore. However, perturbation of Asp141 is observed in the L intermediate at 250 K but not at 170 K. We named these photoproducts La (at 170 K) and Lb (at 250 K). The spectrum of Lb is distinct from that of La also in the different shifts of water O-H stretching bands, and larger changes in the bands from the protein backbone with different sensitivities to varying the halide. These results suggest that the photocycle of halorhodopsin contains two L states, La and Lb, in which the structure of protein and internal water molecules is different but chloride stays at the same site close to the Schiff base.

Bacteriorhodopsins↗

Photochemistry of the primary event in short-wavelength visual opsins at low temperature.

Two short-wavelength cone opsins, frog (Xenopus laevis) violet and mouse UV, were expressed in mammalian COS1 cells, purified in delipidated form, and studied using cryogenic UV-vis spectrophotometry. At room temperature, the X. laevis violet opsin has an absorption maximum at 426 nm when generated with 11-cis-retinal and an absorption maximum of 415 nm when generated with 9-cis-retinal. The frog short-wavelength opsin has two different batho intermediates, one stable at 30 K (lambda(max) approximately 446 nm) and the other at 70 K (lambda(max) approximately 475 nm). Chloride ions do not affect the absorption maximum of the violet opsin. At room temperature, mouse UV opsin has an absorption maximum of 357 nm, while at 70 K, the pigment exhibits a bathochromic shift to 403 nm with distinct vibronic structure and a strong secondary vibronic band at 380 nm. We have observed linear relationships when analyzing the energy difference between the initial and bathochromic intermediates and the normalized difference spectra of the batho-shifted intermediates of rod and cone opsins. We conclude that the binding sites of these pigments change from red to green to violet via systematic shifts in the position of the primary counterion relative to the protonated Schiff base. The mouse UV cone opsin does not fit this trend, and we conclude that wavelength selection in this pigment must operate via a different molecular mechanism. We discuss the possibility that the mouse UV chromophore is initially unprotonated.

Absorption↗

Structural investigation of the active site in bacteriorhodopsin: geometric constraints on the roles of Asp-85 and Asp-212 in the proton-pumping mechanism from solid state NMR.

Constraints on the proximity of the carboxyl carbons of the Asp-85 and Asp-212 side chains to the 14-carbon of the retinal chromophore have been established for the bR(555), bR(568), and M(412) states of bacteriorhodopsin (bR) using solid-state NMR spectroscopy. These distances were examined via (13)C-(13)C magnetization exchange, which was observed in two-dimensional RF-driven recoupling (RFDR) and spin diffusion experiments. A comparison of relative RFDR cross-peak intensities with simulations of the NMR experiments yields distance measurements of 4.4 +/- 0.6 and 4.8 +/- 1.0 A for the [4-(13)C]Asp-212 to [14-(13)C]retinal distances in bR(568) and M(412), respectively. The spin diffusion data are consistent with these results and indicate that the Asp-212 to 14-C-retinal distance increases by 16 +/- 10% upon conversion to the M-state. The absence of cross-peaks from [14-(13)C]retinal to [4-(13)C]Asp-85 in all states and between any [4-(13)C]Asp residue and [14-(13)C]retinal in bR(555) indicates that these distances exceed 6.0 A. For bR(568), the NMR distance constraints are in agreement with the results from recent diffraction studies on intact membranes, while for the M state the NMR results agree with theoretical simulations employing two bound waters in the region of the Asp-85 and Asp-212 residues. The structural information provided by NMR should prove useful for refining the current understanding of the role of aspartic acid residues in the proton-pumping mechanism of bR.

Anisotropy↗