Proton Pump Bacteriorhodopsin Research Articles

Coupling Between the Retinal Thermal Isomerization and the Glu194 Residue of Bacteriorhodopsin†

Glu194 is a residue located at the end of F helix on the extracellular side of the light-induced proton pump bacteriorhodopsin (BR). Currently, it is well recognized that Glu194 and Glu204 residues, along with water clusters, constitute the proton release group of BR. Here we report that the replacement of Glu194 for Gln affects not only the photocycle of the protein but also has tremendous effect on the all-trans to 13-cis thermal isomerization. We studied the pH dependence of the dark adaptation of the E194Q mutant and performed HPLC analysis of the isomer compositions of the light- and partially dark-adapted states of the mutant at several pH values. Our data confirmed that E194Q exhibits extremely slow dark adaptation over a wide range of pH. HPLC data showed that a significantly larger concentration of all-trans isomer was present in the samples of the E194Q mutant even after prolonged dark adaptation. After 14 days in the dark the 13-cis to all-trans ratio was 1:3 in the mutant, compared to 2:1 in the wild type. These data clearly indicate the involvement of Glu194 in control of the rate of all-trans to 13-cis thermal isomerization.

Mutations in Cys 128 cause extreme decelerations of the Channelrhodopsin-2 kinetics

Channelrhodopsin-2 (ChR2) triggers the phototaxis of the green algae Chlamydomonas reinhardtii. Amino acids 1-315 form a Bacteriorhodopsin (BR)-like heptahelical membrane domaine, which comprises the ion permeability and the covalently bound retinal chromophore. Depending on the electrochemical gradients, protons and cations are conducted in both directions upon light activation of ChR2. However, only little is known about the residues that determine the channel function, while proton pumping BR has characterized in almost any detail. In order to ensure a unidirectional charge transfer, BR goes through a photocycle with separated proton uptake and release in which only one proton is pumped. In contrast, Channelrhodopsins conduct hundreds of ions during each cycle. Hence, we deduce that these proteins are approaching a defined photointermediate which forms an open channel pore, i.e. the conducting state. By Two Electrode Voltage Clamp (TEVC) measurments in Xenopus oocytes, we identified an amino acid that plays a crucial role in this process. Mutation of C128 in Helix3 to Thr, Ala or Ser, decelerates the ChR2 kinetics dramatically. For instance, the on-kinetics of C128A is 10 times slower and the off-kinetics even 2000 times slower compared to the wilde type. In addition, we show that cells expressing these mutants are more than 300 times more light-sensitive than ChR2-WT and that they can be used as photo-switches. In BR, a corresponding threonine (BR-Thr90) is located near the 11-12 position of the retinal and is involved in the rearrangement of the α-helices during the photocycle1. We conclude that Cys 128 is critical for both fast opening anf fast closing of the of the ion channelpore.1. Joh, N. H., Min, A., Faham, S., Whitelegge, J. P., Yang, D., Woods, V. L., and Bowie, J. U. (2008) Nature 453, 1266-1270

Flagellar Rotation in the Archaeon Halobacterium salinarum Depends on ATP

Halobacterium salinarum swims with the help of a polarly inserted flagellar bundle. In energized cells, the flagellar motors rotate continuously, occasionally switching the rotational sense. Starving cells become immotile as the energy level drops. Presumably, there is a threshold of energy required for flagellar rotation. When starved, immotile cells are energized by exposure to light, the speed of flagellar rotation increases gradually to its steady state over several minutes. Since the light-driven proton pump bacteriorhodopsin energizes the cell membrane to the maximal level within a fraction of a second, the delay in reaching the maximal swimming speed suggests that the halobacterial flagellar motor may not be driven directly by proton motive force. Swimming cells, which obtain their energy exclusively through light-driven proton pumping, become immotile within 20 min when treated with N,N'-dicyclohexylcarbodiimide (DCCD), an inhibitor of the proton translocating ATP synthase. However, flagellar motility in DCCD-treated cells can be restored by the addition of L-arginine, which serves as a fermentative energy source and restores the cytoplasmic ATP level in the presence of DCCD. This suggests that flagellar motor rotation depends on ATP, and this is confirmed by the observation that motility is increased strongly by L-arginine at zero proton motive force levels. The flagellar motor may be driven either by ATP directly or by an ATP-generated ion gradient that is not coupled directly to the proton gradient or the proton motive force of the cell.

The Lifetimes of Pharaonis Phoborhodopsin Signaling States Depend on the Rates of Proton Transfers—Effects of Hydrostatic Pressure and Stopped Flow Experiments†

Pharaonis phoborhodopsin (ppR), a negative phototaxis receptor of Natronomonas pharaonis, undergoes photocycle similar to the light-driven proton pump bacteriorhodopsin (BR), but the turnover rate is much slower due to much longer lifetimes of the M and O intermediates. The M decay was shown to become as fast as it is in BR in the L40T/F86D mutant. We examined the effects of hydrostatic pressure on the decay of these intermediates. For BR, pressure decelerated M decay but slightly affected O decay. In contrast, with ppR and with its L40T/F86D mutant, pressure slightly affected M decay but accelerated O decay. Clearly, the pressure-dependent factors for M and O decay are different in BR and ppR. In order to examine the deprotonation of Asp75 in unphotolyzed ppR we performed stopped flow experiments. The pH jump-induced deprotonation of Asp75 occurred with 60 ms, which is at least 20 times slower than deprotonation of the equivalent Asp85 in BR and about 10-fold faster than the O decay of ppR. These data suggest that proton transfer is slowed not only in the cytoplasmic channel but also in the extracellular channel of ppR and that the light-induced structural changes in the O intermediate of ppR additionally decrease this rate.

Terahertz radiation from bacteriorhodopsin reveals correlated primary electron and proton transfer processes

The kinetics of electrogenic events associated with the different steps of the light-induced proton pump of bacteriorhodopsin is well studied in a wide range of time scales by direct electric methods. However, the investigation of the fundamental primary charge translocation phenomena taking place in the functional energy conversion process of this protein, and in other biomolecular assemblies using light energy, has remained experimentally unfeasible because of the lack of proper detection technique operating in the 0.1- to 20-THz region. Here, we show that extending the concept of the familiar Hertzian dipole emission into the extreme spatial and temporal range of intramolecular polarization processes provides an alternative way to study ultrafast electrogenic events on naturally ordered biological systems. Applying a relatively simple experimental arrangement based on this idea, we were able to observe light-induced coherent terahertz radiation from bacteriorhodopsin with femtosecond time resolution. The detected terahertz signal was analyzed by numerical simulation in the framework of different models for the elementary polarization processes. It was found that the principal component of the terahertz emission can be well described by excited-state intramolecular electron transfer within the retinal chromophore. An additional slower process is attributed to the earliest phase of the proton pump, probably occurring by the redistribution of a H bond near the retinal. The correlated electron and proton translocation supports the concept, assigning a functional role to the light-induced sudden polarization in retinal proteins.

Electrically insulating pore-suspending membranes on highly ordered porous obtained from vesicle spreading.

Pore-suspending membranes on porous alumina substrates with pore diameters of 60 nm were prepared by fusion of vesicles on a (cholesterylpolyethylenoxy)thiol-functionalized surface, and their functionality demonstrated by the activity of the proton pump bacteriorhodopsin.

Glycocardiolipin modulates the surface interaction of the proton pumped by bacteriorhodopsin in purple membrane preparations

Glycocardiolipin is an archaeal analogue of mitochondrial cardiolipin, having an extraordinary affinity for bacteriorhodopsin, the photoactivated proton pump in the purple membrane of Halobacterium salinarum. Here purple membranes have been isolated by osmotic shock from either cells or envelopes of Hbt. salinarum. We show that purple membranes isolated from envelopes have a lower content of glycocardiolipin than standard purple membranes isolated from cells. The properties of bacteriorhodopsin in the two different purple membrane preparations are compared; although some differences in the absorption spectrum and the kinetic of the dark adaptation process are present, the reduction of native membrane glycocardiolipin content does not significantly affect the photocycle (M-intermediate rise and decay) as well as proton pumping of bacteriorhodopsin. However, interaction of the pumped proton with the membrane surface and its equilibration with the aqueous bulk phase are altered.

Functional Bionetworks from Nanoliter Water Droplets

We form networks from aqueous droplets by submerging them in an oil/lipid mixture. When the droplets are joined together, the lipid monolayers surrounding them combine at the interface to form a robust lipid bilayer. Various protein channels and pores can incorporate into the droplet-interface bilayer (DIB), and the application of a potential with electrodes embedded within the droplets allows ionic currents to be driven across the interface and measured. By joining droplets in linear or branched geometries, functional bionetworks can be created. Although the interfaces between neighboring droplets comprise only single lipid bilayers, the structures of the networks are long-lived and robust. Indeed, a single droplet can be "surgically" excised from a network and replaced with a new droplet without rupturing adjacent DIBs. Networks of droplets can be powered with internal "biobatteries" that use ion gradients or the light-driven proton pump bacteriorhodopsin. Besides their interest as coupled protocells, the droplets can be used as devices for ultrastable bilayer recording with greatly reduced electrolyte volume, which will permit their use in rapid screening applications.

Photochromism ofAnabaenaSensory Rhodopsin

Protein-controlled photochemical reactions often mediate biological light-signal and light-energy conversions. Microbial rhodopsins possess all-trans or 13-cis retinal as the chromophore in the dark, and in the light-driven proton pump, bacteriorhodopsin (BR), the stable photoproduct at the end of the functional cycle of the all-trans form is 100% all-trans. In contrast, a microbial rhodopsin discovered in Anabaena PCC7120 is believed to function as a photochromic sensor. For Anabaena sensory rhodopsin (ASR), the photoreaction is expected to be not cyclic, but photochromic. The present low-temperature UV-visible spectroscopy of ASR indeed revealed that the stable photoproduct of the all-trans form in ASR is 100% 13-cis, and that of the 13-cis form is 100% all-trans. The complete photocycle for the proton pump in BR and the complete photochromism for the chromatic sensor of ASR are highly advantageous for their functions. Thus, the microbial rhodopsins have acquired unique photoreactions, in spite of their similar structures, during evolution.

Structures and spectral signatures of protonated water networks in bacteriorhodopsin.

Networks of internal water molecules are thought to provide proton transfer pathways in many enzymatic and photosynthetic reactions. Extremely broad absorption continua observed in recent IR spectroscopic measurements on the photodriven proton pump bacteriorhodopsin (BR) suggest such networks may also serve as proton storage and release sites for these reactions. By combining electronic structure calculations with molecular mechanical force fields, we examine the dynamics and the resulting IR spectra of two protonated water networks, H+.(H2O)3 and H+.(H2O)4, in the release pocket of the initial state of BR, which possibly serve as proton donors to the extracellular surface. For both network sizes, topologically similar structures are found, which are anchored at residues E194 and E204 and stabilized by additional hydrogen bonds from neighboring protein side chains. These protonated water networks assume neither the classic Zundel nor Eigen motives but prefer wire-like topologies. Upon gauging calculated IR spectra of finite clusters with experimental gas-phase data, it is possible to link spectral features computed for these chain-like structures in the initial state of the BR photocycle to the measured absorption continua, in particular for the larger H+.(H2O)4 network. Furthermore, the free energy of proton dislocation along these chains is found to be within the range that is easily accessible at room temperature because of fluctuations.

External electric control of the proton pumping in bacteriorhodopsin

Comparative analysis of the photoelectric response of dried films of purple membranes (PM) depending on their degree of orientation is presented. Time dependence of the photo-induced protein electric response signal (PERS) of oriented and non-oriented films to a single laser pulse in the presence of the external electric field (EEF) was experimentally determined. The signal does not appear in the non-oriented films when the EEF is absent, whereas the PERS of the oriented PM films demonstrates the variable polarity on the microsecond time scale. In the presence of the EEF the PERS of the non-oriented film rises exponentially preserving the same polarization. The polarization of the PERS changes by changing the polarity of the EEF with no influence on the time constant of the PERS kinetics. The EEF effect on the PERS of the oriented films is more complicated. By subtracting the PERS when EEF not equal 0 from the PERS when EEF = 0 the resulting signal is comparable to that of the non-oriented films. Generalizing the experimental data we conclude that the EEF influence is of the same origin for the films of any orientation. To explain the experimental results the two-state model is suggested. It assumes that the EEF directionally changes the pK(a) values of the Schiff base (SB) and of the proton acceptor aspartic acid D85 in bacteriorhodopsin. Because of that the SB-->D85 proton transfer might be blocked and consequently the L-->M intermediate transition should vanish. Thus, on the characteristic time scale tau( L --> M ) approximately 30 micros; both intermediates, the M intermediate, appearing under normal conditions, and the L intermediate as persisting under the blocked conditions when D85 is protonated, should coexist in the film. The total PERS is a result of the potentials corresponding to the electrogenic products of intermediates L and M that are of the opposite polarity. It is concluded that the ratio of bacteriorhodopsin concentrations corresponding to the L and M intermediates is driven by the EEF and, consequently, it should define the PERS of the non-oriented films. According to this model the orientation degree of the film could be evaluated by describing the PERS.

Conformational Coupling between the Cytoplasmic Carboxylic Acid and the Retinal in a Fungal Light-Driven Proton Pump

Many fungal rhodopsins, eukaryotic structural homologues of the archaeal light-driven proton pump bacteriorhodopsin, have been discovered in the course of genome sequencing projects. Recently, two fungal rhodopsins were characterized in vitro and exhibited very different photochemical behavior. Neurospora rhodopsin possesses a slow photocycle and shows no ion transport, reminiscent of sensory rhodopsins, while Leptosphaeria rhodopsin has a fast bacteriorhodopsin-like photocycle and pumps protons light-dependently. Such a dramatic difference is surprising considering the very high degree of sequence homology of the two proteins. In this paper, we investigate whether the chemical structure of a cytoplasmic carboxylic acid, the homologue of Asp-96 of bacteriorhodopsin serving as a proton donor for the retinal Schiff base, can define the photochemical properties of fungal rhodopsins. We studied mutants of Leptosphaeria rhodopsin in which this aspartic acid was replaced with Glu or Asn using spectroscopy in the infrared and visible ranges. We show that Glu at this position is inefficient as a proton donor similar to a nonprotonatable Asn. Moreover, this replacement induces long-range structural perturbations of the retinal environment, as evidenced by changes in the vibrational bands of retinal (especially, hydrogen-out-of-plane modes) and neighboring aspartic acids and water molecules. The conformational coupling of the mutation site to the retinal may be mediated by helical rearrangements as suggested by the changes in amide and proline vibrational bands. We conclude that the difference in the photochemical behavior of fungal rhodopsins from Leptosphaeria and Neurospora may be ascribed, to some extent, to the replacement of the cytoplasmic proton donor Asp with Glu.

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.

Hydrogen-Bonding Interaction of the Protonated Schiff Base with Halides in a Chloride-Pumping Bacteriorhodopsin Mutant

Bacteriorhodopsin (BR) and halorhodopsin (HR) are light-driven proton and chloride ion pumps, respectively, in Halobacterium salinarum. The amino acid identity of these proteins is about 25%, suggesting that each has been optimized for their own functions during evolution. However, it is known that the BR mutants, D85T and D85S, can pump chloride ions. This fact implies that the Schiff base region is important in determining ionic selectivity. The X-ray crystallographic structure of D85S(Br(-)) showed the presence of a bromide ion in the Schiff base region (Facciotti, M. T., Cheung, V. S., Nguyen, D., Rouhani, S., and Glaeser, R. M. (2003) Biophys. J. 85, 451-458). In this article, we report on the study of hydrogen bonds of the Schiff base and water molecules in D85S in the absence and presence of various halides, assigning their N-D and O-D stretching vibrations in D(2)O, respectively, in low-temperature Fourier-transform infrared (FTIR) spectroscopy. We found that the hydrogen bond of the Schiff base in D85S(Cl(-)) is much stronger than that in HR, being as strong as that in wild-type BR. Similar halide dependence in D85S and in solution implies that the Schiff base forms a direct hydrogen bond with a halide, consistent with the X-ray structure. Photoisomerization causes a weakened hydrogen bond of the Schiff base, and halide dependence on the stretching frequency is lost. These spectral features are similar to those in the photocycle of proton-pumping BR, though the weakened hydrogen bond is more significant for BR. However, the spectral features of water bands in D85S are closer to chloride-pumping HR because O-D stretching vibrations of water are observed only at >2500 cm(-)(1). Unlike in BR, we did not observe strongly hydrogen-bonded water molecules for halide-pumping D85S mutants. This observation agrees with our recent hypothesis that strongly hydrogen-bonded water molecules are required for the proton-pumping activity of archaeal rhodopsins. Hydrogen-bonding conditions in the Schiff base region of D85S are discussed on the basis of the spectral comparison with those of wild-type BR and HR.

Color Tuning in Rhodopsins: The Mechanism for the Spectral Shift between Bacteriorhodopsin and Sensory Rhodopsin II

The mechanism of color tuning in the rhodopsin family of proteins has been studied by comparing the optical properties of the light-driven proton pump bacteriorhodopsin (bR) and the light detector sensory rhodopsin II (sRII). Despite a high structural similarity, the maximal absorption is blue-shifted from 568 nm in bR to 497 nm in sRII. The molecular mechanism of this shift is still a matter of debate, and its clarification sheds light onto the general mechanisms of color tuning in retinal proteins. The calculations employ a combined quantum mechanical/molecular mechanical (QM/MM) technique, using a DFT-based method for ground state properties and the semiempirical OM2/MRCI method and ab initio SORCI method for excited state calculations. The high efficiency of the methodology has allowed us to study a wide variety of aspects including dynamical effects. The absorption shift as well as various mutation experiments and vibrational properties have been successfully reproduced. Our results indicate that several sources contribute to the spectral shift between bR and sRII. The main factors are the counterion region at the extracellular side of retinal and the amino acid composition of the binding pocket. Our analysis allows a distinction and identification of the different effects in detail and leads to a clear picture of the mechanism of color tuning, which is in good agreement with available experimental data.

Low-energy dynamics and biological function

Results from QENS experiments using a resolution of 93 μ e V on a biological system are reported. The photocycle of the proton pump bacteriorhodopsin (BR) is known to slow down with decreasing temperature and humidity, a behaviour related to the ‘dynamic transition’. We have achieved a separation of the pure thermal activation effect involving the plasticizing action of hydration water, from effects due to the variation of the hydration level on the dynamics of purple membrane (PM) with its integral protein BR, and have correlated this with its ability to function. This demonstrates that the biological function of BR requires molecular dynamics in the ps range.

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.

Structural and energetic determinants of primary proton transfer in bacteriorhodopsin

In the light-driven bacteriorhodopsin proton pump, the first proton transfer step is from the retinal Schiff base to a nearby carboxylate group. The mechanism of this transfer step is highly controversial, in particular whether a direct proton jump is allowed. Here, we review the structural and energetic determinants of the direct proton transfer path computed by using a combined quantum mechanical/molecular mechanical approach. Both protein flexibility and electrostatic interactions play an important role in shaping the proton transfer energy profile. Detailed analysis of the energetics of putative transitions in the first half of the photocycle focuses on two elements that determine the likelihood that a given configuration of the active site is populated during the proton-pumping cycle. First, the rate-limiting barrier for proton transfer must be consistent with the kinetics of the photocycle. Second, the active-site configuration must be compatible with a productive overall pumping cycle.

Light Activation of Channelrhodopsin-2 in Excitable Cells of Caenorhabditis elegans Triggers Rapid Behavioral Responses

For studying the function of specific neurons in their native circuitry, it is desired to precisely control their activity. This often requires dissection to allow accurate electrical stimulation or neurotransmitter application , and it is thus inherently difficult in live animals, especially in small model organisms. Here, we employed channelrhodopsin-2 (ChR2), a directly light-gated cation channel from the green alga Chlamydomonas reinhardtii, in excitable cells of the nematode Caenorhabditis elegans, to trigger specific behaviors, simply by illumination. Channelrhodopsins are 7-transmembrane-helix proteins that resemble the light-driven proton pump bacteriorhodopsin , and they also utilize the chromophore all-trans retinal, but to open an intrinsic cation pore. In muscle cells, light-activated ChR2 evoked strong, simultaneous contractions, which were reduced in the background of mutated L-type, voltage-gated Ca2+-channels (VGCCs) and ryanodine receptors (RyRs). Electrophysiological analysis demonstrated rapid inward currents that persisted as long as the illumination. When ChR2 was expressed in mechanosensory neurons, light evoked withdrawal behaviors that are normally elicited by mechanical stimulation. Furthermore, ChR2 enabled activity of these neurons in mutants lacking the MEC-4/MEC-10 mechanosensory ion channel . Thus, specific neurons or muscles expressing ChR2 can be quickly and reversibly activated by light in live and behaving, as well as dissected, animals.

QM/MM investigation of the hydrogen-bonding interactions in putative K and early-M intermediates of the bacteriorhodopsin photocycle

The light-driven photocycle of the bacteriorhodopsin proton pump contains several intermediate states characterized by their spectroscopic signals. Numerous experimental investigations, including high-resolution X-ray crystallography, have provided valuable insight into the nature and the extent of the structural rearrangements along the photocycle. Nevertheless, the detailed hydrogen-bonding interactions of the retinal Schiff base and of the groups involved in proton transfer remain under debate. Combined Quantum Mechanical/Molecular Mechanical (QM/MM) calculations are employed here to assess the hydrogen-bonding interactions in the retinal binding pocket of putative K and early-M stable structures. In both of the starting coordinate sets the retinal chain is highly twisted, with the Schiff base pointing towards the extracellular side of the membrane. The optimization of either the K or the early-M state structure by considering the Schiff base protonated and Asp85 negatively charged (i.e., as in the K intermediate) preserves the highly twisted configuration of the retinal chain. In the case where the optimizations are performed with neutral Schiff base and neutral Asp85 (i.e., as in the M intermediate) the chromophore relaxes and the Schiff base orients towards the cytoplasm. The twisted retinal configuration with the deprotonated Schiff base pointing towards the extracellular side of the membrane is found to be unstable.