Spectroscopic and photochemical characterization of a deep ocean proteorhodopsin

A second group of proteorhodopsin-encoding genes (blue-absorbing proteorhodopsin, BPR) differing by 20-30% in predicted primary structure from the first-discovered green-absorbing (GPR) group has been detected in picoplankton from Hawaiian deep sea water. Here we compare BPR and GPR absorption spectra, photochemical reactions, and proton transport activity. The photochemical reaction cycle of Hawaiian deep ocean BPR in cells is 10-fold slower than that of GPR with very low accumulation of a deprotonated Schiff base intermediate in cells and exhibits mechanistic differences, some of which are due to its glutamine residue rather than leucine at position 105. In contrast to GPR and other characterized microbial rhodopsins, spectral titrations of BPR indicate that a second titratable group, in addition to the retinylidene Schiff base counterion Asp-97, modulates the absorption spectrum near neutral pH. Mutant analysis confirms that Asp-97 and Glu-108 are proton acceptor and proton donor, respectively, in retinylidene Schiff base proton transfer reactions during the BPR photocycle as previously shown for GPR, but BPR contains an alternative acceptor evident in its D97N mutant, possibly the same as the second titratable group modulating the absorption spectrum. BPR, similar to GPR, carries out outward light-driven proton transport in Escherichia coli vesicles but with a reduced translocation rate attributable to its slower photocycle. In energized E. coli cells at physiological pH, the net effect of BPR photocycling is to generate proton currents dominated by a triggered proton influx, rather than efflux as observed with GPR-containing cells. Reversal of the proton current with the K+-ionophore valinomycin supports that the influx is because of voltage-gated channels in the E. coli cell membrane. These observations demonstrate diversity in photochemistry and mechanism among proteorhodopsins. Calculations of photon fluence rates at different ocean depths show that the difference in photocycle rates between GPR and BPR as well as their different absorption maxima may be explained as an adaptation to the different light intensities available in their respective marine environments. Finally, the results raise the possibility of regulatory (i.e. sensory) rather than energy harvesting functions of some members of the proteorhodopsin family.     

His-75 in Proteorhodopsin, a Novel Component in Light-driven Proton Translocation by Primary Pumps

Proteorhodopsins (PRs), photoactive retinylidene membrane proteins ubiquitous in marine eubacteria, exhibit light-driven proton transport activity similar to that of the well studied bacteriorhodopsin from halophilic archaea. However, unlike bacteriorhodopsin, PRs have a single highly conserved histidine located near the photoactive site of the protein. Time-resolved Fourier transform IR difference spectroscopy combined with visible absorption spectroscopy, isotope labeling, and electrical measurements of light-induced charge movements reveal participation of His-75 in the proton translocation mechanism of PR. Substitution of His-75 with Ala or Glu perturbed the structure of the photoactive site and resulted in significantly shifted visible absorption spectra. In contrast, His-75 substitution with a positively charged Arg did not shift the visible absorption spectrum of PR. The mutation to Arg also blocks the light-induced proton transfer from the Schiff base to its counterion Asp-97 during the photocycle and the acid-induced protonation of Asp-97 in the dark state of the protein. Isotope labeling of histidine revealed that His-75 undergoes deprotonation during the photocycle in the proton-pumping (high pH) form of PR, a reaction further supported by results from H75E. Finally, all His-75 mutations greatly affect charge movements within the PR and shift its pH dependence to acidic values. A model of the proteorhodopsin proton transport process is proposed as follows: (i) in the dark state His-75 is positively charged (protonated) over a wide pH range and interacts directly with the Schiff base counterion Asp-97; and (ii) photoisomerization-induced transfer of the Schiff base proton to the Asp-97 counterion disrupts its interaction with His-75 and triggers a histidine deprotonation.A variety of unicellular microorganisms contain primary proton pumps that convert solar energy into a transmembrane electrochemical proton gradient, which is subsequently used by membrane ATP synthases to generate chemical energy. Well known examples of such pumps are the haloarchaeal rhodopsins, photoactive, seven-helix membrane proteins, which include the well studied proton pump bacteriorhodopsin (BR)⁴ from Halobacterium salinarum and BR homologs in other haloarchaea. Recently, a much larger new family of light-driven proton pumps, the proteorhodopsins (PRs), was identified in marine proteobacteria throughout the oceans (1–3). Despite the diverse properties of PRs, including different visible absorption maxima and photocycle rates (4–6), they all share with BR several key conserved residues as well as an all-trans-retinylidene chromophore in their unphotolyzed state, which is covalently bound to transmembrane helix G via a protonated Schiff base linkage.Many of the molecular events that occur in PRs following light activation are similar to those of BR, including an initial ultrafast all-trans→13-cis-retinal isomerization, which triggers a sequence of protein conformational changes, including several intramolecular proton transfer reactions. The two key carboxylate groups involved in proton pumping in helix C of BR are conserved in PRs, and in the first found and most commonly studied PR, the Monterey Bay variant eBAC31A08, also known as green-absorbing proteorhodopsin (GPR), the helix C residues Asp-97 and Glu-108 undergo protonation changes during the photocycle similar to those of the homologous carboxylate residues in BR. Initial FTIR studies on GPR identified the role of Asp-97 as the Schiff base counterion and proton acceptor during Schiff base deprotonation and concomitant M formation and Glu-108 as the proton donor that reprotonates the Schiff base during N formation (7, 8). Studies of other variants indicate these roles of the two carboxylic acid residues are general in the proteorhodopsin family.⁵One major difference between BR and the PRs is the presence of a highly conserved histidine residue at position 75, near the middle of transmembrane helix B in the latter pigments. The His-75 homolog is not present in BR nor thus far found in other microbial rhodopsins (9). The proximity of His-75 to the protein active site and specifically to the Schiff base counterion Asp-97 inferred from the x-ray crystal structure of BR suggests its involvement in spectral tuning of the visible absorption (10) and potentially PR photochemical reactions. Because the pK_a of histidine in solution is close to neutral pH (11), its imidazole group often plays a major role in intramolecular proton transfers in enzymes, including NADPH oxidase (12), alcohol dehydrogenase (13), carbonic anhydrase II (14), and serine proteases (15).In this study we have used a combination of time-resolved FTIR difference spectroscopy, visible absorption spectroscopy, isotope labeling, kinetic charge displacement measurements, and site-directed mutagenesis to study the role of His-75 in GPR. We report evidence that protonated His-75 interacts directly with Asp-97 in the unphotolyzed protein and during the photocycle undergoes a deprotonation in response to the protonation of Asp-97.     

Proteorhodopsin is a light-driven proton pump with variable vectoriality

Proteorhodopsin, a homologue of archaeal bacteriorhodopsin (BR), belongs to a newly identified family of retinal proteins from marine bacteria, which could play an important role in the energy balance of the biosphere. We cloned the cDNA sequence of proteorhodopsin by chemical gene synthesis, expressed the protein in Escherichia coli cells, purified and reconstituted the protein in its functional active state. The photocycle characteristics were determined by time-resolved absorption and Fourier transform infrared (FT-IR) spectroscopy. The pH-dependence of the absorption spectrum indicates that the pK(a) of the primary acceptor of the Schiff base proton (Asp97) is 7.68. Generally, the photocycle of proteorhodopsin is similar to that of BR, although an L-like photocycle intermediate was not detectable. Whereas at pH>7 an M-like intermediate is formed upon illumination, at pH 5 no M-like intermediate could be detected. As the photocycle kinetics do not change between the acidic and alkaline state of proteorhodopsin, the only difference between these two forms is the protonation status of Asp97. This is corroborated by time-resolved FT-IR spectroscopy, which demonstrates that proton transfer from the retinal Schiff base to Asp97 is observed at alkaline pH, but the other vibrational changes are essentially pH-independent.After reconstitution into proteoliposomes, light-induced proton currents of proteorhodopsin were measured in a compound membrane system where proteoliposomes were adsorbed to planar lipid bilayers. Our results show that proteorhodopsin is a light-driven proton pump with characteristics similar to those of BR at alkaline pH. However, at acidic pH, the direction of proton pumping is inverted. Complementary experiments were carried out on proteorhodopsin expressed heterologously in Xenopus laevis oocytes under voltage clamp conditions.The following results were obtained. (1) At alkaline pH, proteorhodopsin mediates outwardly directed proton pumping like BR. (2) The direction of proton pumping can be inverted, when Asp97 is protonated. (3) The current can be inverted by changes of the polarity of the applied voltage. (4) The light intensity-dependence of the photocurrents leads to the conclusion that the alkaline form of proteorhodopsin shows efficient proton pumping after sequential excitation by two photons.     

Voltage- and pH-Dependent Changes in Vectoriality of Photocurrents Mediated by Wild-type and Mutant Proteorhodopsins upon Expression in Xenopus Oocytes

Proteorhodopsin (PR), a light-driven proton pump from marine proteobacteria, exhibits photocycle characteristics similar to bacteriorhodopsin (BR) at neutral pH, including an M-like photointermediate. However, at acidic pH, spectroscopic evidence for an M-like species was absent, and the vectoriality of proton pumping was inverted. To gain further insight into this unusual property, we examined the voltage dependence of stationary and laser flash-induced photocurrents of PR under different pH conditions upon expression in Xenopus oocytes. The current-voltage curves were linear under all conditions tested, and photocurrent reversal potentials distinctly depended on the pH gradient. PR mutants D97N and D97T exhibited transient and stationary inward currents already at neutral pH, showing that neutralization of the proton acceptor abolishes forward pumping and permits only inward proton transport. Mutation E108G, which disrupts the donor site for Schiff base (SB) reprotonation, resulted in largely reduced photocurrents, which could be strongly stimulated by azide, similar to previous observations on BR mutant D96G. When PR and BR photocurrents in response to blue or green laser flashes during or after continuous illumination were compared, direct electrical evidence for the occurrence of an M-like intermediate at neutral pH could only be obtained when reprotonation of the SB was slowed down by PR mutation E108G. For PR at acidic pH, laser flashes only produced inwardly directed photocurrents, independent from background illumination, thus precluding electrical identification of an M-like species. However, when visible absorption spectroscopy was carried out at low temperatures, occurrence of an M-like species was robustly observed at low pH. This indicates that SB deprotonation and reprotonation occur during the PR photocycle also at low pH. Our results corroborate the conclusion that in PR, the direction of proton pumping can be switched by changes in pH and membrane potential, with the protonation state of Asp-97 being the key determinant for selecting between transport modes.     

Proton transfers in the photochemical reaction cycle of proteorhodopsin

The spectral and photochemical properties of proteorhodopsin (PR) were determined to compare its proton transport steps to those of bacteriorhodopsin (BR). Static and time-resolved measurements on wild-type PR and several mutants were done in the visible and infrared (FTIR and FT-Raman). Assignment of the observed C=O stretch bands indicated that Asp-97 and Glu-108 serve as the proton acceptor and donor, respectively, to the retinal Schiff base, as do the residues at corresponding positions in BR, but there are numerous spectral and kinetic differences between the two proteins. There is no detectable dark-adaptation in PR, and the chromophore contains nearly entirely all-trans retinal. Because the pK(a) of Asp-97 is relatively high (7.1), the proton-transporting photocycle is produced only at alkaline pH. It contains at least seven transient states with decay times in the range from 10 micros to 200 ms, but the analysis reveals only three distinct spectral forms. The first is a red-shifted K-like state. Proton release does not occur during the very slow (several milliseconds) rise of the second, M-like, intermediate, consistent with lack of the residues facilitating extracellular proton release in BR. Proton uptake from the bulk, presumably on the cytoplasmic side, takes place prior to release (tau approximately 2 ms), and coincident with reprotonation of the retinal Schiff base. The intermediate produced by this process contains 13-cis retinal as does the N state of BR, but its absorption maximum is red-shifted relative to PR (like the O state of BR). The decay of this N-like state is coupled to reisomerization of the retinal to all-trans, and produces a state that is O-like in its C-C stretch bands, but has an absorption maximum apparently close to that of unphotolyzed PR.     

Photochemical reaction cycle and proton transfers in Neurospora rhodopsin.

It was recently found that NOP-1, a membrane protein of Neurospora crassa, shows homology to haloarchaeal rhodopsins and binds retinal after heterologous expression in Pichia pastoris. We report on spectroscopic properties of the Neurospora rhodopsin (NR). The photocycle was studied with flash photolysis and time-resolved Fourier-transform infrared spectroscopy in the pH range 5-8. Proton release and uptake during the photocycle were monitored with the pH-sensitive dye, pyranine. Kinetic and spectral analysis revealed six distinct states in the NR photocycle, and we describe their spectral properties and pH-dependent kinetics in the visible and infrared ranges. The phenotypes of the mutant NR proteins, D131E and E142Q, in which the homologues of the key carboxylic acids of the light-driven proton pump bacteriorhodopsin, Asp-85 and Asp-96, were replaced, show that Glu-142 is not involved in reprotonation of the Schiff base but Asp-131 may be. This implies that, if the NR photocycle is associated with proton transport, it has a low efficiency, similar to that of haloarchaeal sensory rhodopsin II. Fourier-transform Raman spectroscopy revealed unexpected differences between NR and bacteriorhodopsin in the configuration of the retinal chromophore, which may contribute to the less effective reprotonation switch of NR.     

Membrane potential stabilizes the O intermediate in liposomes containing bacteriorhodopsin.

In the bacteriorhodopsin-containing proteoliposomes, a laser flash is found to induce formation of a bathointermediate decaying in several seconds, the difference spectrum being similar to the purple-blue transition. Different pH buffers do not affect the intermediate, whereas an uncoupler, gramicidin A, and lipophilic ions accelerate decay of the intermediate or inhibit its formation. In the liposomes containing E204Q bacteriorhodopsin mutant, formation of the intermediate is suppressed. In the wild-type bacteriorhodopsin liposomes, the bathointermediate formation is pH-independent within the pH 5-7 range. The efficiency of the long-lived O intermediate formation increases at a low pH. In the wild-type as well as in the E204Q mutant purple membrane, the O intermediate decay is slowed down at slightly higher pH values than that of the purple-blue transition. It is suggested that the membrane potential affects the equilibrium between the bacteriorhodopsin ground state (Glu-204 is protonated and Asp-85 is deprotonated) and the O intermediate (Asp-85 is protonated and Glu-204 is deprotonated), stabilizing the latter by changing the relative affinity of Asp-85 and Glu-204 to H(+). At a low pH, protonation of a proton-releasing group (possibly Glu-194) in the bacteriorhodopsin ground state seems to prevent deprotonation of the Glu-204 during the photocycle. Thus, all protonatable residues of the outward proton pathway should be protonated in the O intermediate. Under such conditions, membrane potential stabilization of the O intermediate in the liposomes can be attributed to the direct effect of the potential on the pK value of Asp-85.     

The proton release group of bacteriorhodopsin controls the rate of the final step of its photocycle at low pH

The factors determining the pH dependence of the formation and decay of the O photointermediate of the bacteriorhodopsin (bR) photocycle were investigated in the wild-type (WT) pigment and in the mutants of Glu-194 and Glu-204, key residues of the proton release group (PRG) in bR. We have found that in the WT the rate constant of O --> bR transition decreases 30-fold upon decreasing the pH from 6 to 3 with a pKa of about 4.3. D2O slows the rise and decay of the O intermediate in the WT at pH 3.5 by a factor of 5.5. We suggest that the rate of the O --> bR transition (which reflects the rate of deprotonation of the primary proton acceptor Asp-85) at low pH is controlled by the deprotonation of the PRG. To test this hypothesis, we studied the E194D mutant. We show that the pKa of the PRG in the ground state of the E194D mutant, when Asp-85 is protonated, is increased by 1.2 pK units compared to that of the WT. We found a similar increase in the pKa of the rate constant of the O --> bR transition in E194D. This provides further evidence that the rate of the O --> bR transition is controlled by the PRG. In a further test, the E194Q mutation, which disables the PRG and slows proton release, almost completely eliminates the pH dependence of O decay at pHs below 6. A second phenomenon we investigated was that in the WT at neutral and alkaline pH the fraction of the O intermediate decreases with pKa 7.5. A similar pH dependence is observed in the mutants in which the PRG is disabled, E194Q and E204Q, suggesting that the decrease in the fraction of the O intermediate with pKa ca. 7.5 is not controlled by the PRG. We propose that the group with pKa 7.5 is Asp-96. The slowing of the reprotonation of Asp-96 at high pH is the cause of the decrease in the rate of the N --> O transition, leading to the decrease in the fraction of O.     

Low temperature FTIR spectroscopy provides new insights in the pH-dependent proton pathway of proteorhodopsin

In the presented study the low pH photocycle of proteorhodopsin is extensively investigated by means of low temperature FTIR spectroscopy. Besides the already well-known characteristics of the all-trans and 13-cis retinal vibrations the 77K difference spectrum at pH 5.1 shows an additional negative signal at 1744 cm(-1) which is interpreted as indicator for the L state. The subsequent photocycle steps are investigated at temperatures higher than 200K. The combination of visible and FTIR spectroscopy enabled us to observe that the deprotonation of the Schiff base is linked to the protonation of an Asp or Glu side chain - the new proton acceptor under acidic conditions. The difference spectra of the late intermediates are characterized by large amide I changes and two further bands ((-)1751 cm(-1)/(+)1725 cm(-1)) in the spectral region of the Asp/Glu ν(C=O) vibrations. The band position of the negative signature points to a transient deprotonation of Asp-97. In addition, the pH dependence of the acidic photocycle was investigated. The difference spectra at pH 5.5 show distinct differences connected to changes in the protonation state of key residues. Based on our data we propose a three-state model that explains the complex pH dependence of PR.     

The photochemical reaction cycle of proteorhodopsin at low pH

The proton acceptor group in the recently described retinal protein, proteorhodopsin has an unusually high pK(a) of 7.1. It was shown that at pH above this pK(a), illumination initiates a photocycle similar to that of bacteriorhodopsin, and the protein transports proton across the cell membrane. Recently it was reported that proteorhodopsin, unlike bacteriorhodopsin, transports protons at pH below the pK(a) of the proton acceptor, and this transport is in the reverse direction. We have investigated the photocycle of proteorhodopsin at such low pH. At pH 5, three spectrally distinct intermediates K, L, and N, and another spectrally silent one, PR', could be identified, but a deprotonated Schiff base containing M-like intermediate, characteristic for proton pumping activity, does not accumulate. All the reactions between the intermediates are close to equilibrium, except the last transition from PR' to PR, when the protein returns to its initial unexcited state in a quasiunidirectional reaction. The electric signal measurements indicate that although charge motions are detected inside the protein, their net dislocation is zero, indicating that contrary to the earlier reported, at low pH no charged particle is transported across the membrane.     

Aspartic acid 85 in bacteriorhodopsin functions both as proton acceptor and negative counterion to the Schiff base.

In bacteriorhodopsin Asp85 has been proposed to function both as a negative counterion to the Schiff base and as proton acceptor in the early stages of the photocycle. To test this proposal further, we have replaced Asp85 by His. The rationale for this replacement is that although His can function as a proton acceptor, it cannot provide a negative charge at residue 85 to serve as a counterion to the protonated Schiff base. We show here that the absorption spectrum of the D85H mutant is highly sensitive to the pH of the external medium. From spectroscopic titrations, we have determined the apparent pK for deprotonation of the Schiff base to be 8.8 +/- 0.1 and the apparent pK for protonation of the His85 side chain to be approximately 3.5. Between pH 3.5 and 8.8, where the Schiff base is protonated, and the His side chain is deprotonated, the D85H mutant is completely inactive in proton transport. Time-resolved studies show that there is no detectable formation of an M-like intermediate in the photocycle of the D85H mutant. These experiments show that the presence of a neutral proton-accepting moiety at residue 85 is not sufficient for carrying out light-driven proton transport. The requirements at residue 85 are therefore for a group that serves both as a negatively charged counterion and as a proton acceptor.     

FTIR spectroscopy of the M photointermediate in pharaonis rhoborhodopsin

pharaonis phoborhodopsin (ppR; also called pharaonis sensory rhodopsin II, psR-II) is a photoreceptor for negative phototaxis in Natronobacterium pharaonis. During the photocycle of ppR, the Schiff base of the retinal chromophore is deprotonated upon formation of the M intermediate (ppR(M)). The present FTIR spectroscopy of ppR(M) revealed that the Schiff base proton is transferred to Asp-75, which corresponds to Asp-85 in a light-driven proton-pump bacteriorhodopsin (BR). In addition, the C==O stretching vibrations of Asn-105 were assigned for ppR and ppR(M). The common hydrogen-bonding alterations in Asn-105 of ppR and Asp-115 of BR were found in the process from photoisomerization (K intermediate) to the primary proton transfer (M intermediate). These results implicate similar protein structural changes between ppR and BR. However, BR(M) decays to BR(N) accompanying a proton transfer from Asp-96 to the Schiff base and largely changed protein structure. In the D96N mutant protein of BR that lacks a proton donor to the Schiff base, the N-like protein structure was observed with the deprotonated Schiff base (called M(N)) at alkaline pH. In ppR, such an N-like (M(N)-like) structure was not observed at alkaline pH, suggesting that the protein structure of the M state activates its transducer protein.     

Protonation/deprotonation reactions triggered by photoactivation of photoactive yellow protein from Ectothiorhodospira halophila.

Light-dependent pH changes were measured in unbuffered solutions of wild type photoactive yellow protein (PYP) and its H108F and E46Q variants, using two independent techniques: transient absorption changes of added pH indicator dyes and direct readings with a combination pH electrode. Depending on the absolute pH of the sample, a reversible protonation as well as a deprotonation can be observed upon formation of the transient, blue-shifted photocycle intermediate (pB) of this photoreceptor protein. The latter is observed at very alkaline pH, the former at acidic pH values. At neutral pH, however, the formation of the pB state is not paralleled by significant protonation/deprotonation of PYP, as expected for concomitant protonation of the chromophore and deprotonation of Glu-46 during pB formation. We interpret these results as further evidence that a proton is transferred from Glu-46 to the coumaric acid chromophore of PYP, during pB formation. One cannot exclude the possibility, however, that this transfer proceeds through the bulk aqueous phase. Simultaneously, an amino acid side chain(s) (e.g. His-108) changes from a buried to an exposed position. These results, therefore, further support the idea that PYP significantly unfolds in the pB state and resolve the controversy regarding proton transfer during the PYP photocycle.     

A large photolysis-induced pKa increase of the chromophore counterion in bacteriorhodopsin: implications for ion transport mechanisms of retinal proteins.

The proton-pumping mechanism of bacteriorhodopsin is dependent on a photolysis-induced transfer of a proton from the retinylidene Schiff base chromophore to the aspartate-85 counterion. Up until now, this transfer was ascribed to a > 7-unit decrease in the pKa of the protonated Schiff base caused by photoisomerization of the retinal. However, a comparably large increase in the pKa of the Asp-85 acceptor also plays a role, as we show here with infrared measurements. Furthermore, the shifted vibrational frequency of the Asp-85 COOH group indicates a transient drop in the effective dielectric constant around Asp-85 to approximately 2 in the M photointermediate. This dielectric decrease would cause a > 40 kJ-mol-1 increase in free energy of the anionic form of Asp-85, fully explaining the observed pK alpha increase. An analogous photolysis-induced destabilization of the Schiff base counterion could initiate anion transport in the related protein, halorhodopsin, in which aspartate-85 is replaced by Cl- and the Schiff base proton is consequently never transferred.     

Lipid membrane mimetics and oligomerization tune functional properties of proteorhodopsin

The functional properties of proteorhodopsin (PR) have been found to be strongly modulated by oligomeric distributions and lipid membrane mimetics. This study aims to distinguish and explain their effects by investigating how oligomer formation impacts PR’s function of proton transport in lipid-based membrane mimetic environments. We find that PR forms stable hexamers and pentamers in both E. coli membranes and synthetic liposomes. Compared with the monomers, the photocycle kinetics of PR oligomers is ～2 and ～4.5 times slower for transitions between the K and M and the M and N photointermediates, respectively, indicating that oligomerization significantly slows PR’s rate of proton transport in liposomes. In contrast, the apparent pKa of the key proton acceptor residue D97 (pKa_D97) of liposome-embedded PR persists at 6.2–6.6, regardless of cross-protomer modulation of D97, suggesting that the liposome environment helps maintain PR’s functional activity at neutral pH. By comparison, when extracted directly from E. coli membranes into styrene-maleic acid lipid particles, the pKa_D97 of monomer-enriched E50Q PR drastically increases to 8.9, implying that there is a very low active PR population at neutral pH to engage in PR’s photocycle. These findings demonstrate that oligomerization impacts PR’s photocycle kinetics, while lipid-based membrane mimetics strongly affect PR’s active population via different mechanisms.     

The role of water in the extracellular half channel of bacteriorhodopsin.

The changes in the photocycle of the wild type and several mutant bacteriorhodopsin (D96N, E204Q, and D212N) were studied on dried samples, at relative humidities of 100% and 50%. Samples were prepared from suspensions at pH approximately 5 and at pH approximately 9. Intermediate M with unprotonated Schiff base was observed at the lower humidity, even in the case where the photocycle in suspension did not contain this intermediate (mutant D212N, high pH). The photocycle of the dried sample stopped at intermediate M1 in the extracellular conformation; conformation change, switching the accessibility of the Schiff base to the cytoplasmic side, and proton transport did not occur. The photocycle decayed slowly by dissipating the absorbed energy of the photon, and the protein returned to its initial bacteriorhodopsin state, through several M1-like substates. These substates presumably reflect different paths of the proton back to the Schiff base, as a consequence of the bacteriorhodopsin adopting different conformations by stiffening on dehydration. All intermediates requiring conformational change were hindered in the dried form. The concentration of intermediate L, which appears after isomerization of the retinal from all-trans to 13-cis, during local relaxation of the protein, was unusually low in dried samples. The lack of intermediates N and O demonstrated that the M state did not undergo a change from the extracellular to the cytoplasmic conformation (M1 to M2 transition), as already indicated by Fourier transform infrared spectroscopy, quasielastic incoherent neutron scattering, and electric signal measurements described in the literature.     

Photocycle in the M-form in bacteriorhodopsin mutants devoid of primary proton acceptor Asp-85

Photoinduced changes in absorption of the deprotonated M-form in the mutant bacteriorhodopsin without primary proton acceptor Asp-85 were studied and additional evidence in support of the complete transmembrane proton transfer in photocycle was obtained. Measurements of the absorption spectrum were carried out at various pH, temperature, and humidity. The direction of proton transfer was the same as in the normal photocycle of the wild-type bacteriorhodopsin: from the internal to the external side of the membrane. The effect on this process of a terminal acceptor Glu-204 was shown.     

Structural changes in bacteriorhodopsin during the photocycle measured by time-resolved polarized Fourier transform infrared spectroscopy.

The structural changes in bacteriorhodopsin during the photocycle are investigated. Time resolved polarized infrared spectroscopy in combination with photoselection is used to determine the orientation and motion of certain structural units of the molecule: Asp-85, Asp-96, Asp-115, the Schiff base, and several amide I vibrations. The results are compared with recently published x-ray diffraction data with atomic resolution about conformational motions during the photocycle. The orientation of the measured vibrations are also calculated from the structure data, and based on the comparison of the values from the two techniques new information is obtained: several amide I bands in the infrared spectrum are assigned, and we can also identify the position of the proton in the protonated Asp residues.     

Study of intermediate N using mutant forms of bacteriorhodopsin at Asp-96]

It has been found that the N(P, R)-type intermediate of the photocycle is formed in the Asp-96-->Asn mutant at acidic pH. Azide, which strongly activates the M decay in this mutant, allows the N intermediate to be shown also at neutral pH. Under these conditions mutant N decays in a pH-independent fashion. In the presence of azide, the H+ uptake by Asp-96-->Asn mutant bacteriorhodopsin follows the M decay, whereas the N decay occurs at a much slower rate. Two electrogenic stages have been shown to be associated with the M--->bR step in the Asp-96--->Asn mutant photocycle. The faster and slower stages correlate with the M--->N and N--->bR transitions, respectively. In the Asp-96--->Asn mutant, high concentrations of azide are found to increase the M decay rate up to the values higher than those in the wild-type protein, both with or without azide. Such an effect is absent for the Asp-96-->Glu mutant. The activation energies for M--->N and N--->bR transitions in the wild-type protein are equal to 18 and 19 kcal x mole-1, respectively. In the Asp-96-->Asn mutant without azide, the activation energy of the M decay is only 5 kcal x mole-1, whereas in the presence of azide in this mutant the activation energies for M and N decays are 8 and 9 kcal x mole-1, respectively. A scheme of events accompanying the Schiff base reprotonation during the photocycle is discussed.     

Protonation state of Glu142 differs in the green- and blue-absorbing variants of proteorhodopsin

Proteorhodopsins are a recently discovered class of microbial rhodopsins, ubiquitous in marine bacteria. Over 4000 variants have thus far been discovered, distributed throughout the oceans of the world. Most variants fall into one of two major groups, green- or blue-absorbing proteorhodopsin (GPR and BPR, respectively), on the basis of both the visible absorption maxima (530 versus 490 nm) and photocycle kinetics ( approximately 20 versus approximately 200 ms). For a well-studied pair, these differences appear to be largely determined by the identity of a single residue at position 105 (leucine/GPR and glutamine/BPR). We find using a combination of visible and infrared spectroscopy that a second difference is the protonation state of a glutamic acid residue located at position 142 on the extracellular side of helix D. In BPR, Glu142 (the GPR numbering system is used) is deprotonated and can act as an alternate proton acceptor, thus explaining the earlier observations that neutralization of the Schiff base counterion, Asp97, does not block the formation of the M intermediate. In contrast, Glu142 in GPR is protonated and cannot act in this state as an alternate proton acceptor for the Schiff base. On the basis of these findings, a mechanism is proposed for proton pumping in BPR. Because the pKa of Glu142 is near the pH of its native marine environment, changes in pH may act to modulate its function in the cell.