Retinal Photoisomerization Research Articles

Modelling time-resolved two-dimensional electronic spectroscopy of the primary photoisomerization event in rhodopsin.

Time-resolved two-dimensional (2D) electronic spectra (ES) tracking the evolution of the excited state manifolds of the retinal chromophore have been simulated along the photoisomerization pathway in bovine rhodopsin, using a state-of-the-art hybrid QM/MM approach based on multiconfigurational methods. Simulations of broadband 2D spectra provide a useful picture of the overall detectable 2D signals from the near-infrared (NIR) to the near-ultraviolet (UV). Evolution of the stimulated emission (SE) and excited state absorption (ESA) 2D signals indicates that the S1 → SN (with N ≥ 2) ESAs feature a substantial blue-shift only after bond inversion and partial rotation along the cis → trans isomerization angle, while the SE rapidly red-shifts during the photoinduced skeletal relaxation of the polyene chain. Different combinations of pulse frequencies are proposed in order to follow the evolution of specific ESA signals. These include a two-color 2DVis/NIR setup especially suited for tracking the evolution of the S1 → S2 transitions that can be used to discriminate between different photochemical mechanisms of retinal photoisomerization as a function of the environment. The reported results are consistent with the available time-resolved pump–probe experimental data, and may be used for the design of more elaborate transient 2D electronic spectroscopy techniques.

FTIR Spectroscopy of a Light-Driven Compatible Sodium Ion-Proton Pumping Rhodopsin at 77 K

Krokinobacter eikastus rhodopsin 2 (KR2) is a light-driven sodium ion pump that was discovered in marine bacteria. Although KR2 is able to pump lithium ions similarly, it is converted into a proton pump in potassium chloride or salts of larger cations. In this paper, we applied light-induced difference Fourier-transform infrared (FTIR) spectroscopy to KR2, a compatible sodium ion-proton pump, at 77 K. The first structural study of the functional cycle showed that the structure and structural changes in the primary processes of KR2 are common to all microbial rhodopsins. The red shifted K formation (KR2K) was accompanied by retinal photoisomerization from an all-trans to a 13-cis form, resulting in a distorted retinal chromophore. The observed hydrogen out-of-plane vibrations were H/D exchangeable, indicating that the chromophore distortion by retinal isomerization is located near the Schiff base region in KR2. This tendency was also the case for bacteriorhodopsin and halorhodopsin but not the case for sensory rhodopsin I and II. Therefore, ion pumps such as proton, chloride, and sodium pumps exhibit local structural perturbations of retinal at the Schiff base moiety, while photosensors show more extended structural perturbations of retinal. The retinal Schiff base of KR2 forms a hydrogen bond that is stronger than in BR. KR2 possesses more protein-bound water molecules than other microbial rhodopsins and contains strongly hydrogen-bonded water (O-D stretch at 2333 cm(-1) in D2O). The light-induced difference FTIR spectra at 77 K were identical between the two states functioning as light-driven sodium ion and proton pumps, indicating that the structural changes in the primary processes are identical between different ion pump functions in KR2. In other words, it is unknown which ions are transported by molecules when they absorb photons and photoisomerize. It is likely that the relaxation processes from the K state lead to an alternative function, namely a sodium ion pump or proton pump, depending on the environment.

Modelling retinal chromophores photoisomerization: from minimal models in vacuo to ultimate bidimensional spectroscopy in rhodopsins

Retinal chromophores are the photoactive molecular units of visual and archaeal rhodopsins, an important class of light-activated biological photoreceptors. Extensive computational studies aimed to reveal the intrinsic photophysical and photochemical behavior of retinals in vacuo and the environmental effects that tune their properties in proteins and in solution are reviewed. Multiconfigurational and multireference perturbative ab initio methods have been used to study retinal models with increasing size, from minimal to unreduced models. The hybrid quantum mechanics/molecular mechanics (QM/MM) approach has been employed for modeling retinals in solution and in proteins. QM/MM studies of the retinal photoisomerization in rhodopsin, a prototype opsin protein responsible for the peripheral vision, have provided fundamental understanding of the electrostatic effects regulating the spectral tuning in proteins and have elucidated the photoisomerization mechanism with atomistic details, consistently with ultrafast optical spectroscopy experiments with sub-20 fs resolution. Different photochemical behaviors are observed for retinals in proteins and in solution. A molecular mechanism involving the interplay between ionic and covalent states during photoisomerization has been hypothesized but it remains uncertain and direct experimental evidences are lacking. Here, we propose transient bidimensional electronic spectroscopy as a conceivable tool for obtaining key information on the retinal photoisomerization in different environments. Combination of computational techniques and ultimate ultrafast spectroscopy experiments could provide fundamental insights on retinals photochemistry and basic understanding for the design of biomimetic photochromic devices.

Protein-Bound Water Molecules in Primate Red- and Green-Sensitive Visual Pigments

Protein-bound water molecules play crucial roles in the structure and function of proteins. The functional role of water molecules has been discussed for rhodopsin, the light sensor for twilight vision, on the basis of X-ray crystallography, Fourier transform infrared (FTIR) spectroscopy, and a radiolytic labeling method, but nothing is known about the protein-bound waters in our color visual pigments. Here we apply low-temperature FTIR spectroscopy to monkey red (MR)- and green (MG)-sensitive color pigments at 77 K and successfully identify water vibrations using D(2)O and D(2)(18)O in the whole midinfrared region. The observed water vibrations are 6-8 for MR and MG, indicating that several water molecules are present near the retinal chromophore and change their hydrogen bonds upon retinal photoisomerization. In this sense, color visual pigments possess protein-bound water molecules essentially similar to those of rhodopsin. The absence of strongly hydrogen-bonded water molecules (O-D stretch at <2400 cm(-1)) is common between rhodopsin and color pigments, which greatly contrasts with the case of proton-pumping microbial rhodopsins. On the other hand, two important differences are observed in water signal between rhodopsin and color pigments. First, the water vibrations are identical between the 11-cis and 9-cis forms of rhodopsin, but different vibrational bands are observed at >2550 cm(-1) for both MR and MG. Second, strongly hydrogen-bonded water molecules (2303 cm(-1) for MR and 2308 cm(-1) for MG) are observed for the all-trans form after retinal photoisomerization, which is not the case for rhodopsin. These specific features of MR and MG can be explained by the presence of water molecules in the Cl(-)-biding site, which are located near positions C11 and C9 of the retinal chromophore. The averaged frequencies of the observed water O-D stretching vibrations for MR and MG are lower as the λ(max) is red-shifted, suggesting that water molecules are involved in the color tuning of our vision.

Coherent control of the isomerization of retinal in bacteriorhodopsin in the high intensity regime

Coherent control protocols provide a direct experimental determination of the relative importance of quantum interference or phase relationships of coupled states along a selected pathway. These effects are most readily observed in the high intensity regime where the field amplitude is sufficient to overcome decoherence effects. The coherent response of retinal photoisomerization in bacteriorhodopsin to the phase of the photoexcitation pulses was examined at fluences of 10(15) - 2.5 × 10(16) photons per square centimeter, comparable to or higher than the saturation excitation level of the S(0) - S(1) retinal electronic transition. At moderate excitation levels of ∼6 × 10(15) photons/cm(2) (<100 GW/cm(2)), chirping the excitation pulses increases the all-trans to 13-cis isomerization yield by up to 16% relative to transform limited pulses. The reported results extend previous weak-field studies [Prokhorenko et al., Science 313, 1257 (2006)] and further illustrate that quantum coherence effects persist along the reaction coordinate in strong fields even for systems as complex as biological molecules. However, for higher excitation levels of ∼200 GW/cm(2), there is a dramatic change in photophysics that leads to multiphoton generated photoproducts unrelated to the target isomerization reaction channel and drastically changes the observed isomerization kinetics that appears, in particular, as a red shift of the transient spectra. These results explain the apparent contradictions of the work by Florean et al. [Proc. Natl. Acad. Sci. U.S.A. 106, 10896 (2009)] in the high intensity regime. We are able to show that the difference in observations and interpretation is due to artifacts associated with additional multiphoton-induced photoproducts. At the proper monitoring wavelengths, coherent control in the high intensity regime is clearly observable. The present work highlights the importance of conducting coherent control experiments in the low intensity regime to access information on quantum interference effects along specific reaction coordinates.

Dependence of Photochemical Reactivity of the All‐trans Retinal Protonated Schiff Base on the Solvent and the Excitation Wavelength

An all-optical experimental technique aimed at measuring photoisomerization quantum yield (phi) of the all-trans protonated Schiff base of retinal in solution has been implemented. Upon the increase in the excitation wavelength from 400 to 540 nm a slight increase in phi from 0.16 +/- 0.03 to 0.20 +/- 0.02 is observed in the chromophore dissolved in methanol, whereas the phi value of the one dissolved in acetonitrile varies only from 0.22 +/- 0.03 (400 nm) to 0.23 +/- 0.04 (540 nm). The results suggest that dissipation of the excited-state vibrational energy excess, along with environment-induced modifications of the potential energy surfaces are necessary for an efficient retinal photoisomerization in both solvent and protein environment.

Protein Fluctuations as the Possible Origin of the Thermal Activation of Rod Photoreceptors in the Dark

Efficient retinal photoisomerization, signal transduction, and amplification contribute to single-photon electrical responses in vertebrates visual cells. However, spontaneous discrete electrical signals arising in the dark, with identical intensity and time profiles as those generated by genuine single photons (dark events), limit the potential capability of the rod visual system to discern single photons from thermal noise. It is accepted that the light and the thermal activation of the rod photoreceptor rhodopsin (Rho) triggers the light and the dark events, respectively. However the activation barrier for the dark events (80-110 kJ/mol) appears to be only half of the barrier for light-dependent activation of Rho (> or =180 kJ/mol). On the basis of these observations, it has been postulated that both processes should follow different pathways, but the molecular mechanism for the thermal activation process still remains an open question and subject of debate. Here, performing infrared difference spectroscopy measurements, we found that the -OH group of Thr118 from bovine Rho exhibits a slow but measurable hydrogen/deuterium exchange (HDX) under native conditions. Given the location of Thr118 in the X-ray structures, isolated from the aqueous phase and in steric contact with the buried retinal chromophore, we assume that a protein structural fluctuation must drive the retinal binding pocket (RBP) transiently open. We characterized the kinetics (rate and activation enthalpy) and thermodynamics (equilibrium constant and enthalpy) of this fluctuation from the global analysis of the HDX of Thr118-OH as a function of the temperature and pH. In parallel, using HPLC chromatography, we determined the kinetics of the thermal isomerization of the protonated 11-cis retinal in solution, as a model for retinal thermal isomerization in an open RBP. Finally, we propose a quantitative two-step model in which the dark activation of Rho is triggered by thermal isomerization of the retinal in a transiently opened RBP, which accurately reproduced both the experimental activation barrier and the rate of the dark events. We conclude that the absolute sensitivity threshold of our visual system is limited by structural fluctuations of the chromophore binding pocket rather than in the chromophore itself.

Low-Temperature FTIR Study of Gloeobacter Rhodopsin: Presence of Strongly Hydrogen-Bonded Water and Long-Range Structural Protein Perturbation upon Retinal Photoisomerization

Gloeobacter rhodopsin (GR) is a light-driven proton-pump protein similar to bacteriorhodopsin (BR), found in Gloeobacter violaceus PCC 7421, a primitive cyanobacterium. In this paper, structural changes of GR following retinal photoisomerization are studied by means of low-temperature Fourier-transform infrared (FTIR) spectroscopy. The initial motivation was to test our hypothesis that proton-pumping rhodopsins possess strongly hydrogen-bonded water molecules in the active center. Water O-D stretching vibrations at <2400 cm(-1) in D(2)O have been regarded as coming from such strongly hydrogen-bonded water, and there is a strong correlation between the proton-pumping activity and the presence of such water molecule. Since GR pumps protons, we expected that GR also possesses strongly hydrogen-bonded water molecule(s), and the FTIR results clearly show that this is indeed the case. In addition, another unexpected finding was gained from the frequency region of protonated carboxylic acids in the GR(K) minus GR spectra at 77 K, where we observed the unique bands of a protonated carboxylic acid at 1735 (+)/1730 (-) cm(-1). Comprehensive mutation study revealed that the vibrational bands originate from the carboxylic C=O stretch of Glu132 at the position corresponding to Asp96 in BR. Glu132 presumably functions as an internal proton donor for the retinal Schiff base, but they may be located far apart (ca. 12 A in BR). The present study demonstrates the long-range structural changes of GR along the proton pathway, even though the protein matrix is frozen at 77 K.

Coherent processes in formation of primary products of rhodopsin photolysis

194 The absorption of the light quantum by rhodopsin (R 498 ), a visual pigment, results in the cis → trans isomerization of its chromophore, 11cis -retinal, over approximately 200 fs [1, 2] with a quantum yield of 0.65 [3]. The physical meaning of this fast and efficient photoreaction is in the maximal utilization of the absorbed light quantum energy for isomerization of 11cis -retinal rather than its dissipation into heat or loss as fluorescence. The isomerization of 11cis -retinal leads to conformational rearrangement in the protein moiety of rhodopsin molecule; as a result, rhodopsin as a G-protein binding receptor acquires the ability to interact with G-protein (transducin), thereby initiating phototransduction in the photoreceptor cell. The dynamics of the 11cis -retinal photoisomerization in rhodopsin has been studied by laser kinetic spectroscopy with a femtosecond resolution [1, 2, 4–6]. It has been demonstrated that the first reaction product, photorhodopsin (photo 570 ), is formed over 200 fs to transform into the next product, bathorhodopsin (batho 535 ), in 2–3 ps [1, 4, 5]. The oscillations of the absorption signals of photo 570 , batho 535 , and initial state R 498 , observed during several picoseconds after excitation, have been also discovered. A high rate and quantum yield of 11cis -retinal photoisomerization in rhodopsin as well as the oscillations of absorption signals of the reaction products suggested that this is a coherent reaction. This means that the photoreaction proceeds via passing of the system through nonstationary oscillation states. In terms of the model of two states [1, 7], when two potential energy surfaces (PESs) are involved in photochemical reaction of rhodopsin (Fig. 1), the corresponding processes can be represented as follows. The action of a femtosecond excitation pulse results in a coherent population of certain oscillatory states in the electron-excited molecule, the set of which is named a coherent oscillatory wave packet (hereinafter, wave packet). The coherent photoreaction can be represented as the movement of wave packet over PES S 1 of the excited state along the reaction coordinate. The reaction products are formed Coherent Processes in Formation of Primary Products of Rhodopsin Photolysis

Gold Nanoparticle Plasmonic Field Effect on the Primary Step of the Other Photosynthetic System in Nature, Bacteriorhodopsin

In regards to the effect of the surface plasmon field of gold nanospheres on the rate of primary steps leading to retinal photoisomerization in the photosynthesis of bacterirhodopsin (bR), it is believed that the light absorption of bR that leads to its retinal isomerization first involves the formation of a highly polar electronic excited state (I460) of the all-trans isomer which strongly polarizes the protein around it. This is followed by its decay to a viibrationally excited 13-cis isomer (J625). The effect of plasmonic field of gold nanospheres of different sizes and concentrations is found to slow down the rate of the isomerization of the polar electronic excited-state to the J625 but has no effect on the vibration relaxation of the isomeric state itself. This is consistent with the electrostatic nature of the plasmonic field.

Subpicosecond Protein Backbone Changes Detected during the Green-Absorbing Proteorhodopsin Primary Photoreaction

Recent studies demonstrate that photoactive proteins can react within several picoseconds to photon absorption by their chromophores. Faster subpicosecond protein responses have been suggested to occur in rhodopsin-like proteins where retinal photoisomerization may impulsively drive structural changes in nearby protein groups. Here, we test this possibility by investigating the earliest protein structural changes occurring in proteorhodopsin (PR) using ultrafast transient infrared (TIR) spectroscopy with approximately 200 fs time resolution combined with nonperturbing isotope labeling. PR is a recently discovered microbial rhodopsin similar to bacteriorhodopsin (BR) found in marine proteobacteria and functions as a proton pump. Vibrational bands in the retinal fingerprint (1175-1215 cm(-1)) and ethylenic stretching (1500-1570 cm(-1)) regions characteristic of all-trans to 13-cis chromophore isomerization and formation of a red-shifted photointermediate appear with a 500-700 fs time constant after photoexcitation. Bands characteristic of partial return to the ground state evolve with a 2.0-3.5 ps time constant. In addition, a negative band appears at 1548 cm(-1) with a time constant of 500-700 fs, which on the basis of total-15N and retinal C15D (retinal with a deuterium on carbon 15) isotope labeling is assigned to an amide II peptide backbone mode that shifts to near 1538 cm(-1) concomitantly with chromophore isomerization. Our results demonstrate that one or more peptide backbone groups in PR respond with a time constant of 500-700 fs, almost coincident with the light-driven retinylidene chromophore isomerization. The protein changes we observe on a subpicosecond time scale may be involved in storage of the absorbed photon energy subsequently utilized for proton transport.

Electrostatic and Steric Interactions Determine Bacteriorhodopsin Single-Molecule Biomechanics

Bacteriorhodopsin (bR) is a haloarchaeal membrane protein that converts the energy of single photons into large structural changes to directionally pump protons across purple membrane. This is achieved by a complex combination of local dynamic interactions controlling bR biomechanics at the submolecular level, producing efficient amplification of the retinal photoisomerization. Using single molecule force spectroscopy at different salt concentrations, we show that tryptophan (Trp) residues use steric specific interactions to create a rigid scaffold in bR extracellular region and are responsible for the main unfolding barriers. This scaffold, which encloses the retinal, controls bR local mechanical properties and anchors the protein into the membrane. Furthermore, the stable Trp-based network allows ion binding to two specific sites on the extracellular loops (BC and FG), which are involved in proton release and lateral transport. In contrast, the cytoplasmic side of bR is mainly governed by relatively weak nonspecific electrostatic interactions that provide the flexibility necessary for large cytoplasmic structural rearrangements during the photocycle. The presence of an extracellular Trp-based network tightly enclosing the retinal seems common to most haloarchaeal rhodopsins, and could be relevant to their exceptional efficiency.

On the mechanism of weak-field coherent control of retinal isomerization in bacteriorhodopsin

Experimental studies of the short time reaction dynamics controlling the chemical branching ratio provide direct evidence for the mechanism of coherent control of the retinal photoisomerization in bacteriorhodopsin in the weak-field limit with respect to the previous report [V. Prokhorenko, A. Nagy, S. Waschuk, L. Brown, R. Birge, R. Miller, Science 313 (2006) 1257]. The phase sensitivity of the reaction dynamics is directly revealed using time- and frequency-resolved pump–probe measurements. The high degree of control of the reaction branching ratio is theoretically explained through a combination of spectral amplitude shaping and phase-dependent coupling to selectively excite vibrations most strongly coupled to the reaction coordinate. Coherent control in this context must involve reaction dynamics that occur on time scales comparable to electronic and vibrational decoherence time scales.

Photocurrent from Oriented Membrane Films Containing Acid-blue and Acid-purple Bacteriorhodopsin and its Mutants

This paper investigates the fast photocurrent components, B1 and B2, from oriented bacteriorhodopsin (BR) membrane films at low pH, under pulsed laser excitation. Adding chloride ion changes the acid-blue BR to its acid-purple form. In the presence of chloride, the acid-purple BR shows a positive B2 component in the same direction as that of BR at neutral pH, indicating a rapid intramolecular charge transfer. In the absence of chloride, the acid-blue BR shows only a negative B1 with multi-components, indicating a rapid charge separation process associated with retinal photoisomerization. The multi-components in B1 are possibly formed due to the heterogeneity of the acid-blue BR. In addition, BR mutants, D85N and D115N, at low pH and in the presence of chloride, generate the B2 component as well. The observation of chloride-dependent B2 component in various cases at low pH, is in favor of a possible transient chloride ion transfer, although the nature of the charge being transferred cannot be identified so far.

FTIR Study of the Retinal Schiff Base and Internal Water Molecules of Proteorhodopsin

Proteorhodopsin (PR), an archaeal-type rhodopsin found in marine bacteria, is a light-driven proton pump similar to bacteriorhodopsin (BR). It is known that Asp97, a counterion of the protonated Schiff base, possesses a higher pKa ( approximately 7) compared to that of homologous Asp85 in BR (<3). This suggests that PR has a hydrogen-bonding network different from that of BR. We previously reported that a strongly hydrogen-bonded water molecule is observed only in the alkaline form of PR, where Asp97 is deprotonated (Furutani, Y., Ikeda, D., Shibata, M., and Kandori, H. (2006) Chem. Phys. 324, 705-708). This is probably correlated with the pH-dependent proton pumping activity of PR. In this work, we studied the water-containing hydrogen-bonding network in the Schiff base region of PR by means of Fourier-transform infrared (FTIR) spectroscopy at 77 K. [zeta-15N]Lys-labeling and 18O water were used for assigning the Schiff base N-D and water O-D stretching vibrations in D2O, respectively. The frequency upshift of the N-D stretch in the primary K intermediate is much smaller for PR than for BR, indicating that the Schiff base forms a hydrogen bond after retinal photoisomerization. We then measured FTIR spectra of the mutants of Asp97 (D97N and D97E) and Asp227 (D227N and D227E) to identify the amino acid interacting with the Schiff base in the K state. The PRK minus PR spectra of D97N and D97E were similar to those of the acidic and alkaline forms, respectively, of the wild type implying that the structural changes upon retinal photoisomerization are not influenced by the mutation at Asp97. In contrast, clear spectral differences were observed in D227N and D227E, including vibrational bands of the Schiff base and water molecules. It is concluded that Asp227 plays a crucial role during the photoisomerization process, though Asp97 acts as the primary counterion in the unphotolyzed state of PR.

Three strategically placed hydrogen-bonding residues convert a proton pump into a sensory receptor.

In haloarchaea, light-driven ion transporters have been modified by evolution to produce sensory receptors that relay light signals to transducer proteins controlling motility behavior. The proton pump bacteriorhodopsin and the phototaxis receptor sensory rhodopsin II (SRII) differ by 74% of their residues, with nearly all conserved residues within the photoreactive retinal-binding pocket in the membrane-embedded center of the proteins. Here, we show that three residues in bacteriorhodopsin replaced by the corresponding residues in SRII enable bacteriorhodopsin to efficiently relay the retinal photoisomerization signal to the SRII integral membrane transducer (HtrII) and induce robust phototaxis responses. A single replacement (Ala-215-Thr), bridging the retinal and the membrane-embedded surface, confers weak phototaxis signaling activity, and the additional two (surface substitutions Pro-200-Thr and Val-210-Tyr), expected to align bacteriorhodopsin and HtrII in similar juxtaposition as SRII and HtrII, greatly enhance the signaling. In SRII, the three residues form a chain of hydrogen bonds from the retinal's photoisomerized C(13)=C(14) double bond to residues in the membrane-embedded alpha-helices of HtrII. The results suggest a chemical mechanism for signaling that entails initial storage of energy of photoisomerization in SRII's hydrogen bond between Tyr-174, which is in contact with the retinal, and Thr-204, which borders residues on the SRII surface in contact with HtrII, followed by transfer of this chemical energy to drive structural transitions in the transducer helices. The results demonstrate that evolution accomplished an elegant but simple conversion: The essential differences between transport and signaling proteins in the rhodopsin family are far less than previously imagined.

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

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

Structural Changes in Bacteriorhodopsin following Retinal Photoisomerization from the 13-Cis Form

Bacteriorhodopsin (BR), a light-driven proton pump in Halobacterium salinarum, accommodates two resting forms of the retinylidene chromophore, the all-trans form (AT-BR) and the 13-cis,15-syn form (13C-BR). Both isomers are present in thermal equilibrium in the dark, but only the all-trans form has proton-pump activity. In this study, we applied low-temperature Fourier-transform infrared (FTIR) spectroscopy to 13C-BR at 77 K and compared the local structure around the chromophore before and after photoisomerization with that in AT-BR. Strong hydrogen-out-of-plane (HOOP) vibrations were observed at 964 and 958 cm(-)(1) for the K state of 13C-BR (13C-BR(K)) versus a vibration at 957 cm(-)(1) for the K state of AT-BR (AT-BR(K)). In AT-BR(K), but not in 13C-BR(K), the HOOP modes exhibit isotope shifts upon deuteration of the retinylidene at C15 and at the Schiff base nitrogen. Whereas the HOOP modes of AT-BR(K) were significantly affected by the mutation of Thr89, this was not the case for the HOOP modes of 13C-BR(K). These observations imply that, while the chromophore distortion is localized near the Schiff base in AT-BR(K), it is located elsewhere in 13C-BR(K). By use of [zeta-(15)N]lysine-labeled BR, we identified the N-D stretching vibrations of the 13C-BR Schiff base (in D(2)O) at 2173 and 2056 cm(-)(1), close in frequency to those of AT-BR. These frequencies indicate strong hydrogen bonding of the Schiff base in 13C-BR, presumably with a water molecule as in AT-BR. In contrast, the N-D stretching vibration appears at 2332 and 2276 cm(-)(1) in 13C-BR(K) versus values of 2495 and 2468 cm(-)(1) for AT-BR(K), suggesting that the rupture of the Schiff base hydrogen bond that occurs in AT-BR(K) does not occur in 13C-BR(K). Rotational motion of the Schiff base upon retinal isomerization is probably smaller in magnitude for 13C-BR than for AT-BR. These differences in the primary step are possibly related to the absence of light-driven proton pumping by 13C-BR.

First Steps of Retinal Photoisomerization in Proteorhodopsin

The early steps (<1 ns) in the photocycle of the detergent solubilized proton pump proteorhodopsin are analyzed by ultrafast spectroscopic techniques. A comparison to the first primary events in reconstituted proteorhodopsin as well as to the well known archaeal proton pump bacteriorhodopsin is given. A dynamic Stokes shift observed in fs-time-resolved fluorescence experiments allows a direct observation of early motions on the excited state potential energy surface. The initial dynamics is dominated by sequentially emerging stretching (<150 fs) and torsional (∼300 fs) modes of the retinal. The different protonation states of the primary proton acceptor Asp-97 drastically affect the reaction rate and the overall quantum efficiencies of the isomerization reactions, mainly evidenced for time scales above 1 ps. However, no major influence on the fast time scales (∼150 fs) could be seen, indicating that the movement out of the Franck-Condon region is fairly robust to electrostatic changes in the retinal binding pocket. Based on fs-time-resolved absorption and fluorescence spectra, ground and exited state contributions can be disentangled and allow to construct a reaction model that consistently explains pH-dependent effects in solubilized and reconstituted proteorhodopsin.

FTIR Study of the Photoisomerization Processes in the 13-cis and All-trans Forms of Anabaena Sensory Rhodopsin at 77 K

Archaeal-type rhodopsins can accommodate either all-trans- or 13-cis,15-syn-retinal in their chromophore binding site in the dark, but only the former isomer is functionally important. In contrast, Anabaena sensory rhodopsin (ASR), an archaeal-type rhodopsin found in eubacteria, exhibits a photochromic interconversion of both forms, suggesting that ASR functions as a photosensor which interacts with its 14 kDa soluble transducer differently in the all-trans and 13-cis,15-syn forms. In this study, we applied low-temperature Fourier transform infrared (FTIR) spectroscopy to the 13-cis,15-syn form of ASR (13C-ASR) at 77 K and compared the local structure around the chromophore and its structural changes upon retinal photoisomerization with those of the all-trans form (AT-ASR) [Furutani, Y., Kawanabe, A., Jung, K. H., and Kandori, H. (2005) Biochemistry 44, 12287-12296]. By use of [zeta-15N]lysine-labeled ASR, we identified the N-D stretching vibrations of the Schiff base (in D2O) at 2165 cm(-1) for 13C-ASR and at 2163 and 2125 cm(-1) for AT-ASR. The frequencies indicate strong hydrogen bonds of the Schiff base with a water molecule for both 13C-ASR and AT-ASR. In contrast, the N-D stretching vibration appears at 2351 cm(-1) and at 2483 cm(-1) for the K states of 13C-ASR (13C-ASR(K)) and AT-ASR (AT-ASR(K)), respectively, indicating that the Schiff base still forms a hydrogen bond in 13C-ASR(K). Rotational motion of the Schiff base upon retinal isomerization is probably smaller for 13C-ASR than for AT-ASR, the latter altering hydrogen bonding of the Schiff base similar to bacteriorhodopsin (BR), a light-driven proton pump. Appearance of several hydrogen-out-of-plane vibrations and amide I vibrations in 13C-ASR(K), but not in AT-ASR(K), suggests that structural changes are distributed widely along the polyene chain for 13C-ASR. On the other hand, retinal photoisomerization in AT-ASR breaks the hydrogen bond of the Schiff base, and localized structural changes in the Schiff base region are induced.