Photoelectric response of polarization sensitive bacteriorhodopsin films

Polarization sensitivity is introduced into oriented bacteriorhodopsin (BR) films through a photochemical bleaching process, which chemically modifies the structure of the purple membrane by breaking the intrinsic symmetry of the membrane-bound BR trimers. The resulting photovoltage generated in an indium-tin oxide (ITO)/BR/ITO detector is found to be anisotropic with respect to cross-polarized probe beams. A model, based on the polarization dependent photoselection of the BR molecules qualitatively explains the photochemical bleaching process and the observed anisotropic response. The effect reported here can be used to construct a polarization sensitive BR-based bio-photoreceiver.     

Temperature dependence of photovoltages generated by bacteriorhodopsin.

The temperature dependence of the photovoltage developed by a model membrane containing bacteriorhodopsin (BR) is studied. The model membrane is formed by first coating a thin Teflon sheet with lipid and then fusing BR vesicles to it. The time course of the photoresponse is resolved down to 1 microsecond. The photoresponse is taken to be a sum of exponentials. Exponential time constants and amplitudes are determined by an analysis of the photoresponse with a photovoltage vs. log time plot, correlation filter, and nonlinear least-squares routine. The photovoltage is taken to be the sum of three exponentials but only two of the three time constants are resolved. Both are temperature dependent and indicate a thermally activated transport process. The corresponding activation energies are 55 kJ/mol and 62 kJ/mol. Since the photovoltage is proportional to charge times displacement the corresponding charge displacements are 11 and 34 A assuming a total displacement of 45 A. The remaining exponential term corresponds to a small negative transient in the photovoltage that has a rise time less than 1 microsecond even at -20 degrees C. The calculated charge displacement is estimated to be less than 2 A.     

细菌视紫红质的光电响应特性和机制

在ITO导电玻璃上制备定向细菌视紫红质 (BR)电泳沉积膜或LB膜组成光电池系统 ,在短脉冲激光照射下 ,测定其脉冲响应光电压 ;在间断光照射下 ,测定其对光强变化产生的微分响应信号。对脉冲光电响应和微分响应的机理及其关系进行理论分析和解释 ,认为脉冲响应是BR分子内部生色团快速光极化引起的电荷分离和希夫碱及其周围氨基酸去质子化和再质子化过程引起的质子定向运输产生的位移电流 ,是一个快反应过程 ,是微分响应的早期反应和基础。微分响应则是由于菌紫质的光驱动质子泵产生的连续质子流在光开和光关瞬间引起光电池系统充放电以及测量电路的耦合特性引起的 ,是一个慢变化过程     

Direct measurement of the photoelectric response time of bacteriorhodopsin via electro-optic sampling

The photovoltaic signal associated with the primary photochemical event in an oriented bacteriorhodopsin film is measured by directly probing the electric field in the bacteriorhodopsin film using an ultrafast electro-optic sampling technique. The inherent response time is limited only by the laser pulse width of 500 fs, and permits a measurement of the photovoltage with a bandwidth of better than 350 GHz. All previous published studies have been carried out with bandwidths of 50 GHz or lower. We observe a charge buildup with an exponential formation time of 1.68 +/- 0.05 ps and an initial decay time of 31.7 ps. Deconvolution with a 500-fs Gaussian excitation pulse reduces the exponential formation time to 1.61 +/- 0.04 ps. The photovoltaic signal continues to rise for 4.5 ps after excitation, and the voltage profile corresponds well with the population dynamics of the K state. The origin of the fast photovoltage is assigned to the partial isomerization of the chromophore and the coupled motion of the Arg-82 residue during the primary event.     

Transient photovoltages in purple membrane multilayers. Charge displacement in bacteriorhodopsin and its photointermediates

The photovoltaic properties of bacteriorhodopsin molecules and their photochemical intermediates have been investigated in an experimental cell consisting of multilayered films of highly oriented, dry fragments of purple membrane and lipid sandwiched between two metal (Pd) electrodes. The electrical time constant of these sandwich cells containing between 5 and 30 layers is less than 10(-5) S. Bright illumination of these cells with actinic flashes of approximately 1 ms duration generates transient photovoltages. These photovoltages, which make the extracellular surface of purple membrane positive with respect to the intracellular surface, follow the time course of the flash with no detectable latency. The amplitude of the photovoltages increases linearly with light intensity and their action spectrum matches the absorption spectrum of the light-adapted state of bacteriorhodopsin, BR570. In these dry multilayer cells, the slow photointermediates of bacteriorhodopsin, M412, N520 and O640 are long lived. Illumination of the sandwich cells with long duration (200 ms) pulses of light results, therefore, in the formation of photomixtures containing all these slow photointermediates. Flash illumination of the sandwich cells immediately following the conditioning pulse produces photovoltages whose action spectra match the absorption spectra of the M412 and N520 photointermediates. The M412 photovoltages, like the BR570 photovoltages, follow the time course of the actinic flash with no detectable latency and increase in amplitude linearly with light intensity. But, unlike the BR570 photovoltage, the M412, N520 and O640 photovoltages make the extracellular surface of purple membrane negative with respect to the intracellular surface. Through the of their specific photovoltaic signals, M412 and N520 are shown to be kinetically distinct photointermediates of bacteriorhodopsin. Detection of fast photovoltages with these characteristics in the absence of any ionic solution, and in parallel with spectrophotometric changes, suggest that they arise from charge displacements in the bacteriorhodopsin molecules and their photointermediates as they undergo photochemical conversion in response to the absorption of photons.     

基因突变细菌视紫红质薄膜的长寿命M态光存储

实验研究了D96N型基因突变细菌视紫红质薄膜的光存储性能,实现了用670 nm激光在BR膜上记录光学图像,用560 nm弱光读出图像,用488 nm激光擦除图像的写读擦操作.M态寿命在室温下延长到了3 min,比溶液状态下的野生细菌视紫红质M态寿命延长了5个数量级.     

Photochemistry of monomethylated and permethylated bacteriorhodopsin.

Methylation of the nonactive site lysines of bacteriorhodopsin to form permethylated bacteriorhodopsin does not interfere with the formation of the short wavelength intermediate M412 or light-induced proton release/uptake. The absorption spectrum is similar to that of the native bacteriorhodopsin. However, additional monomethylation of the active site lysine of bacteriorhodopsin causes a red shift of the absorption maximum from 568 nm in light-adapted bacteriorhodopsin [BR] to 630 nm. The photochemistry of active-site methylated BR does not proceed beyond the L-photointermediate. In particular, the photointermediate corresponding to M412 does not form, and there is no proton pumping. Moreover, there is no tyrosine deprotonation. Thus, the formation of an M-type photointermediate is required for proton pumping by BR.     

Flash kinetic study of the last steps in the photoinduced reaction cycle of bacteriorhodopsin

The reaction cycle of light adapted bacteriorhodopsin (BR) in aqueous purple membrane suspensions was studied by laser flash photolysis at different temperatures (2–49°C) and pH values (3–10). The activation energy for several reaction steps was determined at pH 7.6. The kinetics of O-bacteriorhodopsin (one of the last intermediates in the cycle) were analyzed in some detail and it was found that the simple consecutive reaction scheme M-BR → O-BR → BR may explain the kinetics of O-bacteriorhodopsin as measured at 680 nm. Since the pH change in neutral aqueous suspensions of purple membrane follows a similar kinetics as O-bacteriorhodopsin it is suggested that protons are released during the reaction M-BR → O-BR and taken up again during the reaction O-BR → BR.Another long-lived intermediate, which absorbs to a greater extent than bacteriorhodopsin at 570 nm and less than bacteriorhodopsin at 420 nm, was identified with the strongly fluorescing species, pseudo- or P-bacteriorhodopsin. The decay of P-bacteriorhodopsin in bacteriorhodopsin had an activation energy of only approx. 1.2 kcal/mol, which suggests that the last step of the photocycle is a relaxation around a single bond.At pH 9–10, the simple first-order kinetics of all the intermediates were changed into a kinetics consisting of two first-order decays. This change of kinetics was accompanied by a drastic decrease in the rotational diffusion relaxation time.To explain the results obtained in this work and those of others, a model involving proton uptake and release by the Schiff base nitrogen combined with an isomerization reaction is finally proposed.     

Electrogenic proton-pumping capabilities of the m-fast and m-slow photocycles of bacteriorhodopsin

The parallel model for the bacteriorhodopsin (BR) photocycle at neutral pH and a temperature near 20 degrees C contains an M-fast cycle with steps BR-->K-->L-->Mf-->N-->O-->BR and an M-slow cycle which contains steps BR-->K-->L-->Ms-->BR. With increasing actinic laser strength, the M-fast cycle at first rises faster than the M-slow cycle, but reaches saturation sooner and at a lower level than the M-slow cycle. The O-intermediate shows the same saturation behavior as Mf. In this paper, we show that the peak current of proton flux and the apparent voltages developed by this flux show the same saturation behavior as Ms, which is very different from that of both M f and O. It is further shown that most of the proton-charge displacement is connected with the step Ms-->BR. The optical and electrical data in these studies were collected simultaneously by a newly designed and built spectrometer which is described separately.     

Light-induced, long-lived perturbation of the photocycle of bacteriorhodopsin

The relative weight of the slowly decaying M intermediate of the photocycle of bacteriorhodopsin increases upon increasing the energy density of the short (10 ns) actinic laser pulse. Moreover, when a pre-exciting flash is applied to the BR sample, the absolute amplitude of the Ms is higher in the signal induced by a second flash, applied with a delay from 100 microseconds to 100 ms. These facts together prove that either the leftover BR ground-state population becomes different due to the pre-excitation, or there is a cooperative interaction between the BR molecules.     

Mechanism of Nonlinear Photoinduced Anisotropy in Bacteriorhodopsin and its Derivatives

Polymer films made with photosensitive chromophore protein bacteriorhodopsin (BR) from the extreme halophile Halobacterium salinarium as well as films made with BR derivatives exhibit a nonlinear photoinduced anisotropy. Two different methods can be used to induce anisotropy in polymer BR films. The first method is based on the anisotropic properties of the initial form of the photocycle, BR570 (B-type anisotropy). Another method is based on the anisotropic properties of the longest-lived photocycle intermediate M412 (M-type anisotropy). CW gas lasers were employed to induce a reversible anisotropy in polymer BR films. Nonlinear photoinduced anisotropy is discussed in the context of a model for the anisotropic photoselection of BR molecules under linearly polarized light. A comparison of the experimental dependencies of nonlinear photoinduced anisotropy on laser intensity with similar calculated dependencies enables one to determine the molecular dichroism of BR and its derivatives not only for the initial form of the photocycle, B but also for the longest-lived intermediate M. Here we present the data showing the correlation between the laser induced nonlinear anisotropic properties and chromophore/protein interactions in BR. The effect of polymer binder on the nonlinear photoanisotropic properties of polymer BR films is also described.     

Measuring net protease activities in biological samples using selective peptidic inhibitors

Matrix-assisted laser desorption/ionization mass spectrometry (MALDI-MS) is widely used for analysis of macromolecules like peptides and proteins. The analysis procedure is generally simple but must be adapted to the characteristics of the analytes. Therefore, specific matrices suitable for, e.g., hydrophobic proteins and peptides that are difficult to analyze would be preferable in order to optimize the outcome. In the present work, 2,6-dihydroxyacetophenone (DHAP) was shown to be beneficial in comparison to DHB for intact bacteriorhodopsin (BR) as well as for chemically digested BR.     

Modeling the membrane potential generation of bacteriorhodopsin

The archaeon Halobacterium salinarum can grow phototrophically with only light as its energy source. It uses the retinal containing and light-driven proton pump bacteriorhodopsin to enhance the membrane potential which drives the ATP synthase. Therefore, a model of the membrane potential generation of bacteriorhodopsin is of central importance to the development of a mathematical model of the bioenergetics of H. salinarum. To measure the current produced by bacteriorhodopsin at different light intensities and clamped voltages, we expressed the gene in Xenopus laevis oocytes. We present current-voltage measurements and a mathematical model of the current-voltage relationship of bacteriorhodopsin and its generation of the membrane potential. The model consists of three intermediate states, the BR, L, and M states, and comparisons between model predictions and experimental data show that the L to M reaction must be inhibited by the membrane potential. The model is not able to fit the current-voltage measurements when only the M to BR phase is membrane potential dependent, while it is able to do so when either only the L to M reaction or both reactions (L to M and M to BR) are membrane potential dependent. We also show that a decay term is necessary for modeling the rate of change of the membrane potential.     

On the photocycle and light adaptation of dark-adapted bacteriorhodopsin.

Pulsed Nd laser (25 ns, 530 nm) photolysis experiments were carried out at room temperature in aqueous suspensions of dark- and light-adapted fragments of the purple membrane of Halobacterium halobium. It is shown that the (50%) 13-cis isomeric component (BR13-cis) of dark-adapted bacteriorhodopsin (BRDA) undergoes a photocycle involving a characteristic transient absorbing in the neighborhood of 610 nm. At relatively high excitation intensities BR13-cis is converted to the same 410 nm (M) transient that characterized the photocycle of the all-trans isomer (BRtrans) of light-adapted bacteriorhodopsin (BRLA). This process, which competes with the generation of the "610" species, is attributed to the photo-induced conversion, during the pulse, of BR13-cis (or of its primary photoproduct "X") to a species in the BRtrans photocyte. The relationship between these observations and the mechanism of BRDA hv leads to BRLA adaptation at low excitation intensities (for which a quantum yield limit, 0 less than or equal to (3.5 +/- 0.7) X 10(-2) , is established) is discussed.     

Two-photon absorption of bacteriorhodopsin: formation of a red-shifted thermally stable photoproduct F620

By means of high-intensity 532 nm laser pulses, a photochemical conversion of the initial B(570) state of bacteriorhodopsin (BR) to a stable photoproduct absorbing maximally at approximately 620 nm in BR suspensions and at approximately 610 nm in BR films is induced. This state, which we named F(620), is photochemically further converted to a group of three products with maximal absorptions in the wavelength range from 340 nm to 380 nm, which show identical spectral properties to the so-called P(360) state reported in the literature. The photoconversion from B(570) to F(620) is most likely a resonant two-photon absorption induced step. The formation of F(620) and P(360) leads to a distinguished photo-induced permanent optical anisotropy in BR films. The spectral dependence of the photo-induced anisotropy and the anisotropy orientations at the educt (B(570)) and product (F(620)) wavelengths are strong indicators that F(620) is formed in a direct photochemical step from B(570). The chemical nature of the P(360) products probably is that of a retro-retinal containing BR, but the structural characteristics of the F(620) state are still unclear. The photo-induced permanent anisotropy induced by short laser pulses in BR films helps to better understand the photochemical pathways related to this transition, and it is interesting in view of potential applications as this feature is the molecular basis for permanent optical data storage using BR films.     

Dimeric-like kinetic cooperativity of the bacteriorhodopsin molecules in purple membranes.

The kinetics of the absorption changes accompanying the photocycle of bacteriorhodopsin (BR) strongly depend on the intensity of the exciting short laser pulse. The decrease in the flash intensity dependence of the M kinetics after different extents of bleaching of the purple membranes by hydroxylamine proves the existence of a cooperative interaction between the photocycling BR molecules. The yield of the slow component of the M decay (M(s)) is a quadratic function of the extent of the fraction cycling. The slope of the relative weight of M(s) versus the fraction cycling is 0.5. This slope indicates a dimeric-like cooperative interaction, although the structural units of the purple membranes are the trimers of the BR molecules. For the most probable cooperative mechanism an asymmetric trimeric interaction is suggested, which accounts for the apparently dimeric features. A photocycling molecule may influence only one of its two neighbors in the trimer. From this asymmetric feature a deformative interaction is expected to be the cooperative mechanism, which would be an allosteric regulating mechanism in the purple membrane.     

Bacteriorhodopsin/amphipol complexes: structural and functional properties

The membrane protein bacteriorhodopsin (BR) can be kept soluble in its native state for months in the absence of detergent by amphipol (APol) A8-35, an amphiphilic polymer. After an actinic flash, A8-35-complexed BR undergoes a complete photocycle, with kinetics intermediate between that in detergent solution and that in its native membrane. BR/APol complexes form well defined, globular particles comprising a monomer of BR, a complete set of purple membrane lipids, and, in a peripheral distribution, ∼2 g APol/g BR, arranged in a compact layer. In the absence of free APol, BR/APol particles can autoassociate into small or large ordered fibrils.     

Optical CDMA system using bacteriorhodopsin for optical data storage

An optical CDMA (code division multiple access) system for the optical data storage using bacteriorhodopsin (BR) is reported as an application of the BR materials. The desired signal of multiple input can be recorded and reconstructed by use of orthogonal codes. An experimental setup is proposed and demonstrated.     

The chromophore retinal hinders passive proton/hydroxide ion translocation through bacteriorhodopsin

Experiments have been performed to examine any influence of the chromophore retinal in bacteriorhodopsin (BR) on the passive proton/hydroxide ion flux through this integral membrane protein. BR was reconstituted into dimyristoylphosphatidylcholine (DMPC)-phosphatidylserine or DMPC-dimyristoylphosphatidylglycerol unilamellar vesicles with molar lipid to protein ratios ranging from 30 to 150. The entrapped fluorescence dye pyranine served as a reliable indicator of the internal proton concentration. Transmembrane pH-gradients were quickly established across the vesicular membrane and the kinetics of the induced fluorescence changes were compared for vesicles with incorporated native BR, BR bleached to the chromophore-free protein bacterioopsin, and BR regenerated from bacterioopsin with all-trans-retinal, respectively. For aggregated protein molecules, the H+/OH- diffusion across bacterioopsin was always considerably faster than that through the protein containing covalently bound retinal. The decay rate of the imposed pH-gradient was 4.4-9.1 and 2.0-5.1 times slower for native and regenerated BR, respectively, as compared to bacterioopsin. Stepwise regeneration of bacterioopsin with all-trans-retinal revealed a linear dependence of the predominant delta pH-decay time on the degree of regeneration. Essentially the same observations were made with monomeric protein molecules in vesicular lipid membranes. The results demonstrate that the chromophore retinal itself blocks the H+/OH- conducting pathway across the transmembrane protein BR or indirectly controls this path by inducing conformational changes in the protein upon binding.     

I. Primary electrogenic processes in bacteriorhodopsin probed by photoelectric measurements with capacitative metal electrodes

Purple membranes in suspension were electrically oriented between metal electrodes forming a planar capacitor and the flash-induced charge displacements were measured as a photovoltage. This geometry brought about unprecedented high time resolution, even at low ionic strengths. An electrical transmission window of this capacitative cuvette for open circuit photovoltage was characterized. The photovoltage from purple membranes displayed two phases of opposite polarity. The early negative phase resembled a step function in the submicrosecond range. When excited with picosecond laser flashes, this phase showed an instrumentally limited rise-time of about 380 ps, proving a primary charge separation in bacteriorhodopsin which is faster than or equal to 100 ps. The separated charges are stable for about 1 μs. Within the experimental resolution and within the time range between 380 ps and 1 μs, there was no relaxation which could be attributed to a protein relaxation or to a K′ intermediate. The photovoltage decayed with different time constants of the order of 1 μs, depending on the conductance of the medium. Of the same order were the cell time constant and the time constant of the decay of the spectral K intermediate. This hampered the evaluation of the correlation between the photovoltage and the K-L transition. Another positive phase had a smaller amplitude and displayed a time constant of 30 μs which did not depend on the conductivity of the medium. This phase was approx. 40% faster than the decay of the spectroscopically measured L-intermediate. The latter result indicates that charge displacements occur in the time range of the L-M transition, and are not exactly correlated to spectroscopic transients in the visible range.