Time-resolved photointermediate changes in rhodopsin glutamic acid 181 mutants

The role of glutamic acid 181 in the bovine rhodopsin retinylidene chromophore pocket was studied by expressing E181 mutants in COS cells and measuring, as a function of time, the absorbance changes produced after excitation of lauryl maltoside pigment suspensions with 7 ns laser pulses. All mutants studied except E181D showed accelerated decay of bathorhodopsin compared to wild type. Even for E181D, an anomalously large blue shift was observed in the absorption spectrum of the bathorhodopsin decay product, BSI. These observations support the idea that E181 plays a significant role in the earliest stages of receptor activation. E181 mutations have a pronounced effect on the decay of the lumirhodopsin photointermediate, primarily affecting the size of the red shift that occurs in the lumirhodopsin I to lumirhodopsin II transition that takes place on the 10 micros time scale after wild-type photoexcitation. While the spectral change that occurs in the lumirhodopsin I to lumirhodopsin II transition in wild-type rhodopsin is very small ( approximately 2 nm), making it difficult to detect, it is larger in E181D ( approximately 6 nm), making it evident even in the lower signal-to-noise ratio measurements possible with rhodopsin mutants. The change seen is even larger for the E181F mutant where significant amounts of a deprotonated Schiff base intermediate are produced with the 10 micros time constant of lumirhodopsin II formation. The E181Q mutant shows lumirhodopsin decay more similar to wild-type behavior, and no lumirhodopsin I to lumirhodopsin II transition can be resolved. The addition of chloride ion to E181Q increases the lumirhodopsin I-lumirhodopsin II spectral shift and slows the deprotonation of the Schiff base. The latter result is consistent with the idea that a negative charge at position 181 contributes to protonated Schiff base stability in the later intermediates.     

Proton movement and photointermediate kinetics in rhodopsin mutants

The role of ionizable amino acid side chains in the bovine rhodopsin activation mechanism was studied in mutants E134Q, E134R/R135E, H211F, and E122Q. All mutants exhibited bathorhodopsin stability on the 30 ns to 1 micros time scale similar to that of the wild type. Lumirhodopsin decay was also similar to that of the wild type except for the H211F mutant where early decay (20 micros) to a second form of lumirhodopsin was seen, followed by formation of an extremely long-lived Meta I(480) product (34 ms), an intermediate which forms to a much reduced extent, if at all, in dodecyl maltoside suspensions of wild-type rhodopsin. A smaller amount of a similar long-lived Meta I(480) product was seen after photolysis of E122Q, but E134Q and E134R/R135Q displayed kinetics much more similar to those of the wild type under these conditions (i.e., no Meta I(480) product). These results support the idea that specific interaction of His211 and Glu122 plays a significant role in deprotonation of the retinylidene Schiff base and receptor activation. Proton uptake measurements using bromcresol purple showed that E122Q was qualitatively similar to wild-type rhodopsin, with at least one proton being released during lumirhodopsin decay per Meta I(380) intermediate formed, followed by uptake of at least two protons per rhodopsin bleached on a time scale of tens of milliseconds. Different results were obtained for H211F, E134Q, and E134R/R135E, which all released approximately two protons per rhodopsin bleached. These results show that several ionizable groups besides the Schiff base imine are affected by the structural changes involved in rhodopsin activation. At least two proton uptake groups and probably at least one proton release group in addition to the Schiff base are present in rhodopsin.     

pH dependence of photolysis intermediates in the photoactivation of rhodopsin mutant E113Q

Glutamic acid at position 113 in bovine rhodopsin ionizes to form the counterion to the protonated Schiff base (PSB), which links the 11-cis-retinylidene chromophore to opsin. Photoactivation of rhodopsin requires both Schiff base deprotonation and neutralization of Glu-113. To better understand the role of electrostatic interactions in receptor photoactivation, absorbance difference spectra were collected at time delays from 30 ns to 690 ms after photolysis of rhodopsin mutant E113Q solubilized in dodecyl maltoside at different pH values at 20 degrees C. The PSB form (pH 5. 5, lambda(max) = 496 nm) and the unprotonated Schiff base form (pH 8. 2, lambda(max) = 384 nm) of E113Q rhodopsin were excited using 477 nm or 355 nm light, respectively. Early photointermediates of both forms of E113Q were qualitatively similar to those of wild-type rhodopsin. In particular, early photoproducts with spectral shifts to longer wavelengths analogous to wild-type bathorhodopsin were seen. In the case of the basic form of E113Q, the absorption maximum of this intermediate was at 408 nm. These results suggest that steric interaction between the retinylidene chromophore and opsin, rather than charge separation, plays the dominant role in energy storage in bathorhodopsin. After lumirhodopsin, instead of deprotonating to form metarhodopsin I(380) on the submillisecond time scale as is the case for wild type, the acidic form of E113Q produced metarhodopsin I(480), which decayed very slowly (exponential lifetime = 12 ms). These results show that Glu-113 must be present for efficient deprotonation of the Schiff base and rapid visual transduction in vertebrate visual pigments.     

Tunable laser resonance Raman spectroscopic investigations of the transduction process in vertebrate rod cells.

Tunable laser resonance Raman spectroscopy has been applied to probe (in vivo) the role of rhodopsin in transducing light energy into the chemical necessary to generate a neural response. These in vivo experiments have suggested that the Schiff base linkage through which retinal is attached to opsin in rhodopsin is protonated. Furthermore, it appears that light eventually stimulates the deprotonation of the Schiff base linkage between the Meta I and Meta II steps in the intermediate sequence which is the result of light interacting with rhodopsin. Our data suggest that this deprotonation of the Schiff base occurs on the same time scale as overall proton release and uptake by the rhodopsin molecule. It is interesting to note that this series of protonations and deprotonations also occurs within the same time scale as the neural response generation in vertebrates and the generation of a proton gradient by bacteriorhodopsin, which is used by the bacterium, Halobacterium halobium, for ATP synthesis. If these data are analyzed within the context of the in vivo resonance Raman experiments (which seem to indicate that proton release is stimulated in the disc membrane during transduction) then there is a strong suggestion that the proton will assume an important role in any working hypothesis of visual transduction. In essence it appears that protons along with ATP and calcium ions must all be essential elements in the transduction process.     

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.     

Rhodopsin-lumirhodopsin phototransition of bovine rhodopsin investigated by Fourier transform infrared difference spectroscopy

The rhodopsin-lumirhodopsin transition has been investigated by Fourier transform infrared difference spectroscopy using isotope-labeled retinals. In the transition, two protonated carboxyl groups are involved. Another carbonyl band, located at 1725 cm-1 in rhodopsin, is shifted to 1731.5 cm-1 in lumirhodopsin. This line is tentatively assigned to a carbonyl stretching vibration of a peptide bond adjacent to the nitrogen of a proline residue. The C=N stretching vibration of rhodopsin could unequivocally be assigned to a band at 1659 cm-1. In contrast to rhodopsin and bathorhodopsin, the C=N stretching vibration of lumirhodopsin is at a low position, i.e., at 1635 cm-1, and exhibits only a downshift of 4 cm-1 upon deuteriation of the nitrogen. The C15-H rocking vibration of rhodopsin is assigned to the unusual high position of 1456 cm-1 and shifts into the normal region upon formation of lumirhodopsin. From these results, it is concluded that, whereas the environment of the Schiff base in rhodopsin, bathorhodopsin, and isorhodopsin is approximately the same, large changes occur with the formation of lumirhodopsin. From the assignment of the C10-C11 stretching vibration in bathorhodopsin and lumirhodopsin, a 10-s-cis geometry of lumirhodopsin can be excluded.     

A study of the Schiff base mode in bovine rhodopsin and bathorhodopsin

We have obtained the resonance Raman spectra of bovine rhodopsin, bathorhodopsin, and isorhodopsin for a series of isotopically labeled retinal chromophores. The specific substitutions are at retinal's protonated Schiff base moiety and include -HC = NH+-, -HC = ND+-, -H13C = NH+-, and -H13C = ND+-. Apart from the doubly labeled retinal, we find that the protonated Schiff base frequency is the same, within experimental error, for both rhodopsin and bathorhodopsin for all the substitutions measured here and elsewhere. We develop a force field that accurately fits the observed ethylenic (C = C) and protonated Schiff base stretching frequencies of rhodopsin and labeled derivatives. Using MINDO/3 quantum mechanical procedures, we investigate the response of this force field, and the ethylenic and Schiff base stretching frequencies, to the placement of charges close to retinal's Schiff base moiety. Specifically, we find that the Schiff base frequency should be measurably affected by a 3.0-4.5-A movement of a negatively charged counterion from the positively charged protonated Schiff base moiety. That there is no experimentally discernible difference in the Schiff base frequency between rhodopsin and bathorhodopsin suggests that models for the efficient conversion of light to chemical energy in the rhodopsin to bathorhodopsin photoconversion based solely on salt bridge separation of the protonated Schiff base and its counterion are probably incorrect. We discuss various alternative models and the role of electrostatics in the rhodopsin to bathorhodopsin primary process.     

Removal of the 9-methyl group of retinal inhibits signal transduction in the visual process. A Fourier transform infrared and biochemical investigation

The photoreaction of opsin regenerated with 9-demethylretinal has been investigated by UV-vis spectroscopy, flash photolysis experiments, and Fourier transform infrared difference spectroscopy. In addition, the capability of the illuminated pigment to activate the retinal G-protein has been tested. The photoproduct, which can be stabilized at 77 K, resembles more the lumirhodopsin species, and only minor further changes occur upon warming the sample to 170 K (stabilizing lumirhodopsin). UV-vis spectroscopy reveals no further changes at 240 K (stabilizing metarhodopsin I), but infrared difference spectroscopy shows that the protein as well as the chromophore undergoes further molecular changes which are, however, different from those observed for unmodified metarhodopsin I. UV-vis spectroscopy, flash photolysis experiments, and infrared difference spectroscopy demonstrate that an intermediate different from metarhodopsin II is produced at room temperature, of which the Schiff base is still protonated. The illuminated pigment was able to activate G-protein, as assayed by monitoring the exchange of GDP for GTP gamma S in purified G-protein, only to a very limited extent (approximately 8% as compared to rhodopsin). The results are interpreted in terms of a specific steric interaction of the 9-methyl group of the retinal in rhodopsin with the protein, which is required to initiate the molecular changes necessary for G-protein activation. The residual activation suggests a conformer of the photolyzed pigment which mimics metarhodopsin II to a very limited extent.     

Chromophore structure in lumirhodopsin and metarhodopsin I by time-resolved resonance Raman microchip spectroscopy.

Time-resolved resonance Raman microchip flow experiments have been performed on the lumirhodopsin (Lumi) and metarhodopsin I (Meta I) photointermediates of rhodopsin at room temperature to elucidate the structure of the chromophore in each species as well as changes in protein-chromophore interactions. Transient Raman spectra of Lumi and Meta I with delay times of 16 micros and 1 ms, respectively, are obtained by using a microprobe system to focus displaced pump and probe laser beams in a microfabricated flow channel and to detect the scattering. The fingerprint modes of both species are very similar and characteristic of an all-trans chromophore. Lumi exhibits a relatively normal hydrogen-out-of-plane (HOOP) doublet at 951/959 cm(-1), while Meta I has a single HOOP band at 957 cm(-1). These results suggest that the transitions from bathorhodopsin to Lumi and Meta I involve a relaxation of the chromophore to a more planar all-trans conformation and the elimination of the structural perturbation that uncouples the 11H and 12H wags in bathorhodopsin. Surprisingly, the protonated Schiff base C=N stretching mode in Lumi (1638 cm(-1)) is unusually low compared to those in rhodopsin and bathorhodopsin, and the C=ND stretching mode shifts down by only 7 cm(-1) in D2O buffer. This indicates that the Schiff base hydrogen bonding is dramatically weakened in the bathorhodopsin to Lumi transition. However, the C=N stretching mode in Meta I is found at 1654 cm(-1) and exhibits a normal deuteration-induced downshift of 24 cm(-1), identical to that of the all-trans protonated Schiff base. The structural relaxation of the chromophore-protein complex in the bathorhodopsin to Lumi transition thus appears to drive the Schiff base group out of its hydrogen-bonded environment near Glu113, and the hydrogen bonding recovers to a normal solvated PSB value but presumably a different hydrogen bond acceptor with the formation of Meta I.     

Rhodopsin in nanodiscs has native membrane-like photointermediates

Time-dependent studies of membrane protein function are hindered by extensive light scattering that impedes application of fast optical absorbance methods. Detergent solubilization reduces light scattering but strongly perturbs rhodopsin activation kinetics. Nanodiscs may be a better alternative if they can be shown to be free from the serious kinetic perturbations associated with detergent solubilization. To resolve this, we monitored absorbance changes due to photointermediates formed on the microsecond to hundred millisecond time scale after excitation of bovine rhodopsin nanodiscs and compared them to photointermediates that form in hypotonically washed native membranes as well as to those that form in lauryl maltoside suspensions at 15 and 30 °C over a pH range from 6.5 to 8.7. Time-resolved difference spectra were collected from 300 to 700 nm at a series of time delays after photoexcitation and globally fit to a sum of time-decaying exponential terms, and the photointermediates present were determined from the spectral coefficients of the exponential terms. At the temperatures and pHs studied, photointermediates formed after photoexcitation of rhodopsin in nanodiscs are extremely similar to those that form in native membrane, in particular displaying the normal forward shift of the Meta I(480) ? Meta II equilibrium with increased temperature and reduced pH which occurs in native membrane but which is not observed in lauryl maltoside detergent suspensions. These results were obtained using the amount of rhodopsin in nanodiscs which is required for optical experiments with rhodopsin mutants. This work demonstrates that late, physiologically important rhodopsin photointermediates can be characterized in nanodiscs, which provide the superior optical properties of detergent without perturbing the activation sequence.     

Photoreactions of metarhodopsin III

Meta III is an inactive intermediate thermally formed following light activation of the visual pigment rhodopsin. It is produced from the Meta I/Meta II photoproduct equilibrium of rhodopsin by a thermal isomerization of the protonated Schiff base C=N bond of Meta I, and its chromophore configuration is therefore all-trans 15-syn. In contrast to the dark state of rhodopsin, which catalyzes exclusively the cis to trans isomerization of the C11=C12 bond of its 11-cis 15-anti chromophore, Meta III does not acquire this photoreaction specificity. Instead, it allows for light-dependent syn to anti isomerization of the C15=N bond of the protonated Schiff base, yielding Meta II, and for trans to cis isomerizations of C11=C12 and C9=C10 of the retinal polyene, as shown by FTIR spectroscopy. The 11-cis and 9-cis 15-syn isomers produced by the latter two reactions are not stable, decaying on the time scale of few seconds to dark state rhodopsin and isorhodopsin by thermal C15=N isomerization, as indicated by time-resolved FTIR methods. Flash photolysis of Meta III produces therefore Meta II, dark state rhodopsin, and isorhodopsin. Under continuous illumination, the latter two (or its unstable precursors) are converted as well to Meta II by presumably two different mechanisms.     

Photolysis intermediates of human rhodopsin.

Photochemical studies were conducted on human rhodopsin at 20 degrees C to characterize the intermediates which precede the formation of metarhodopsin II, the trigger for the enzyme cascade mechanism of visual transduction. Human rhodopsin was prepared from eyes which had previously been used for corneal donations. Time resolved absorption spectra collected from 10(-8) to 10(-6) s after photolysis of human rhodopsin in detergent suspensions displayed biexponential decay kinetics. The apparent lifetimes obtained from the data are 65 +/- 20 and 292 +/- 25 ns, almost a factor of 2 slower than the corresponding rates in bovine rhodopsin. The spectra can be fit well using a model in which human bathorhodopsin decays toward equilibrium with a blue-shifted intermediate (BSI) which then decays to lumirhodopsin. Spectra and kinetic rate constants were determined for all these intermediates using a global analysis which showed that the spectra of the human intermediates are remarkably similar to bovine intermediates. Microscopic rate constants derived from this model are 7.4 x 10(6) s-1 for bathorhodopsin decay and 7.5 x 10(6) s-1 and 4.6 x 10(6) s-1 for the forward and reverse reactions of BSI, respectively. Decay of lumirhodopsin to later intermediates was studied from 10(-6) to 10(-1) s after photolysis of rhodopsin in human disk membrane suspensions. The human metarhodopsin I in equilibrium metarhodopsin II equilibrium appears to be more forward shifted than in comparable bovine studies.     

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.     

Octopus photoreceptor membranes. Surface charge density and pK of the Schiff base of the pigments.

The chromophore of octopus rhodopsin is 11-cis retinal, linked via a protonated Schiff base to the protein backbone. Its stable photoproduct, metarhodopsin, has all-trans retinal as its chromphore. The Schiff base of acid metarhodopsin (lambda max = 510 nm) is protonated, whereas that of alkaline metarhodopsin (lambda max = 376 nm) is unprotonated. Metarhodopsin in photoreceptor membranes was titrated and the apparent pK of the Schiff base was measured at different ionic strengths. From these salt-dependent pKs the surface charge density of the octopus photoreceptor membranes and the intrinsic Schiff base pK of metarhodopsin were obtained. The surface charge density is sigma = -1.6 +/- 0.1 electronic charges per 1,000 A2. Comparison of the measured surface charge density with values from octopus rhodopsin model structures suggests that the measured value is for the extracellular surface and so the Schiff base in metarhodopsin is freely accessible to protons from the extracellular side of the membrane. The intrinsic Schiff base pK of metarhodopsin is 8.44 +/- 0.12, whereas that of rhodopsin is found to be 10.65 +/- 0.10 in 4.0 M KCl. These pK values are significantly higher than the pK value around 7.0 for a retinal Schiff base in a polar solvent; we suggest that a plausible mechanism to increase the pK of the retinal pigments is the preorganization of their chromophore-binding sites. The preorganized site stabilizes the protonated Schiff base with respect to the unprotonated one. The difference in the pK for the octopus rhodopsin compared with metarhodopsin is attributed to the relative freedom of the latter's chromophore-binding site to rearrange itself after deprotonation of the Schiff base.     

Transducer-binding and transducer-mutations modulate photoactive-site-deprotonation in sensory rhodopsin I.

Sensory rhodopsin I (SRI) is a seven-transmembrane helix retinylidene protein that mediates color-sensitive phototaxis responses through its bound transducer HtrI in the archaeon Halobacterium salinarum. Deprotonation of the Schiff base attachment site of the chromophore accompanies formation of the SRI signaling state, S(373). We measured the rate of laser flash-induced S(373) formation in the presence and absence of HtrI, and the effects of mutations in SRI or HtrI on the kinetics of this process. In the absence of HtrI, deprotonation occurs rapidly (halftime 10 micros) if the proton acceptor Asp76 is ionized (pK(a) = approximately 7), and only very slowly (halftime > 10 ms) when Asp76 is protonated. Transducer-binding, although it increases the pK(a) of Asp76 so that it is protonated throughout the range of pH studied, results in a first order, pH-independent rate of S(373) formation of approximately 300 micros. Therefore, the complexation of HtrI facilitates the proton-transfer reaction, increasing the rate approximately 50-fold at pH6. Arrhenius analysis shows that HtrI-binding accelerates the reaction primarily by an entropic effect, suggesting HtrI constrains the SRI molecule in the complex. Function-perturbing mutations in SRI and HtrI also alter the rate of S(373) formation and the lambda(max) of the parent state as assessed by laser flash-induced kinetic difference spectroscopy, and shifts to longer wavelength are correlated with slower deprotonation. The data indicate that HtrI affects electrostatic interactions of the protonated Schiff base and not only receives the signal from SRI but also optimizes the photochemical reaction process for SRI signaling.     

Light-induced protein conformational changes in the photolysis of octopus rhodopsin.

Light-induced protein conformational changes in the photolysis of octopus rhodopsin were measured with a highly sensitive time-resolved transient UV absorption spectrophotometer with nanosecond time resolution. A negative band around 280 nm in the lumirhodopsin minus rhodopsin spectra suggests that alteration of the environment of some of the tryptophan residues has taken place before the formation of lumirhodopsin. A small recovery of the absorbance at 280 nm was observed in the transformation of lumirhodopsin to mesorhodopsin. Kinetic parameters suggest that major conformational changes have taken place in the transformation of mesorhodopsin to acid metarhodopsin. In this transformation, drastic changes of amplitude and a shift of a difference absorption band around 280 nm take place, which suggest that some of the tryptophan residues of rhodopsin become exposed to a hydrophilic environment.     

Photoisomerization efficiency in UV-absorbing visual pigments: protein-directed isomerization of an unprotonated retinal Schiff base

A visual pigment consists of an opsin protein and a chromophore, 11-cis-retinal, which binds to a specific lysine residue of opsin via a Schiff base linkage. The Schiff base chromophore is protonated in pigments that absorb visible light, whereas it is unprotonated in ultraviolet-absorbing visual pigments (UV pigments). To investigate whether an unprotonated Schiff base can undergo photoisomerization as efficiently as a protonated Schiff base in the opsin environment, we measured the quantum yields of the bovine rhodopsin E113Q mutant, in which the Schiff base is unprotonated at alkaline pH, and the mouse UV pigment (mouse UV). Photosensitivities of UV pigments were measured by irradiation of the pigments followed by chromophore extraction and HPLC analysis. Extinction coefficients were estimated by comparing the maximum absorbances of the original pigments and their acid-denatured states. The quantum yield of the bovine rhodopsin E113Q mutant at pH 8.2, where the Schiff base is unprotonated, was significantly lower than that of wild-type rhodopsin, whereas the mutant gave a quantum yield almost identical to that of the wild type at pH 5.5, where the Schiff base is protonated. These results suggest that Schiff base protonation plays a role in increasing quantum yield. The quantum yield of mouse UV, which has an unprotonated Schiff base chromophore, was significantly higher than that of the unprotonated form of the rhodopsin E113Q mutant, although it was still lower than the visible-absorbing pigments. These results suggest that the mouse UV pigment has a specific mechanism for the efficient photoisomerization of its unprotonated Schiff base chromophore.     

Low-temperature solid-state 13C NMR studies of the retinal chromophore in rhodopsin

Magic angle sample spinning (MASS) 13C NMR spectra have been obtained of bovine rhodopsin regenerated with retinal prosthetic groups isotopically enriched with 13C at C-5 and C-14. In order to observe the 13C retinal chromophore resonances, it was necessary to employ low temperatures (-15-----35 degrees C) to restrict rotational diffusion of the protein. The isotropic chemical shift and principal values of the chemical shift tensor of the 13C-5 label indicate that the retinal chromophore is in the twisted 6-s-cis conformation in rhodopsin, in contrast to the planar 6-s-trans conformation found in bacteriorhodopsin. The 13C-14 isotropic shift and shift tensor principal values show that the Schiff base C = N bond is anti. Furthermore, the 13C-14 chemical shift (121.2 ppm) is within the range of values (120-123 ppm) exhibited by protonated (C = N anti) Schiff base model compounds, indicating that the C = N linkage is protonated. Our results are discussed with regard to the mechanism of wavelength regulation in rhodopsin.     

Evidence for a bound water molecule next to the retinal Schiff base in bacteriorhodopsin and rhodopsin: a resonance Raman study of the Schiff base hydrogen/deuterium exchange.

The retinal chromophores of both rhodopsin and bacteriorhodopsin are bound to their apoproteins via a protonated Schiff base. We have employed continuous-flow resonance Raman experiments on both pigments to determine that the exchange of a deuteron on the Schiff base with a proton is very fast, with half-times of 6.9 +/- 0.9 and 1.3 +/- 0.3 ms for rhodopsin and bacteriorhodopsin, respectively. When these results are analyzed using standard hydrogen-deuteron exchange mechanisms, i.e., acid-, base-, or water-catalyzed schemes, it is found that none of these can explain the experimental results. Because the exchange rates are found to be independent of pH, the deuterium-hydrogen exchange can not be hydroxyl (or acid-)-catalyzed. Moreover, the deuterium-hydrogen exchange of the retinal Schiff base cannot be catalyzed by water acting as a base because in that case the estimated exchange rate is predicted to be orders of magnitude slower than that observed. The relatively slow calculated exchange rates are essentially due to the high pKa values of the Schiff base in both rhodopsin (pKa > 17) and bacteriorhodopsin (pKa approximately 13.5). We have also measured the deuterium-hydrogen exchange of a protonated Schiff base model compound in aqueous solution. Its exchange characteristics, in contrast to the Schiff bases of the pigments, is pH-dependent and consistent with the standard base-catalyzed schemes. Remarkably, the water-catalyzed exchange, which has a half-time of 16 +/- 2 ms and which dominates at pH 3.0 and below, is slower than the exchange rate of the Schiff base in rhodopsin and bacteriorhodopsin.(ABSTRACT TRUNCATED AT 250 WORDS)