Blue light regeneration of bacteriorhodopsin bleached by continuous light.

Photobleaching of bacteriorhodopsin (BR) by continuous light has recently been demonstrated. This bleaching consists of at least two subsequent product states. One of them is absorbing maximally in the blue spectral region. Our present study shows that upon illumination of the bleached sample with blue light a back photoprocess appears, resulting in regeneration of the original BR state. From a technical point of view, the observed phenomenon is similar to the reverting effect of blue light on the photocycle. An important difference is that the photobleached state of BR is much more stable than any of the photocycle intermediates, and may provide an advantage for several technical applications.

Bleaching of bacteriorhodopsin by continuous light.

A new two step photobleaching process is observed under continuous illumination of bacteriorhodopsin. This photobleaching is considerable even at physiological temperatures and becomes large at 50-60 degrees C. The photobleaching also increases with increasing pH from 7 to 10. We suggest that the bleaching at its final stage could be due to the dissociation of the retinal and a local thermal denaturation-like process. These facts may question the generally held belief that BR is a stable protein in vivo for a long period of time. Our results may have relevance also to practical applications of bacteriorhodopsin where the stability of bacteriorhodopsin is a key issue. In certain instances, the use of bacteriorhodopsin may require cooled conditions. Here, we defined the conditions under which bacteriorhodopsin is stable. The permanent photobleaching offers a new way of picture imaging and information input for bacteriorhodopsin-based optical devices.

Cooperativity-induced optical anisotropy changes during the photocycle of bacteriorhodopsin.

Previous photoselection measurements showed that if the excitation is weak no optical anisotropy changes appear in immobilized purple membranes during the photocycle. The present study demonstrates that surprisingly at stronger excitations the anisotropy changes versus time. At 412 nm the dichroic ratio decreases after a few milliseconds, while at 570 nm the similar decrease is followed by an increase. The phenomenon cannot be described by tiltings of the retinal chromophore. It is the consequence of the cooperative interaction among the photocycling bacteriorhodopsin molecules that regulates the yields of more than one (expectedly two main) parallel pathways existing in the millisecond time domain of the photocycle.

Actinic light density dependence of the O intermediate of the photocycle of bacteriorhodopsin.

The O intermediate of the photocycle of bacteriorhodopsin (BR) was studied by absorption kinetic measurements at different actinic light densities. With increasing exciting flash intensity, the relative yield of O slightly increases, while that of Mf strongly decreases at the expense of Ms. Kinetic calculations and the optical anisotropy of O show that O can be formed only from Mf although Mf and O have different light intensity dependences. In order to resolve the apparent contradiction, a phenomenologically new cooperative regulatory mechanism seems to be necessary.

Influence of excitation energy on the bacteriorhodopsin photocycle.

Kinetic curves for the bacteriorhodopsin (BR) photocycle were obtained both at 570 and at 412 nm at a series of increasing levels of intensity of the exciting laser. Singular value decomposition (SVD) of these curves showed two transitions in the kinetic profiles that occurred at specific levels of actinic light. This means that the photocycle was influenced by photon density in two ways. In a separate application of SVD, time-resolved optical spectra were analyzed at each of many levels of exciting laser intensities. The studies showed that the transition at the low level of laser intensity was due principally to an increase in the amount of BR that was turning over. The transition at the higher level of laser intensity showed a fundamental change in kinetics of the photocycle. At low intensity levels, the fast form of M (Mf) predominated, whereas at high levels the slow form of M (Ms) predominated. A distinction was found between Mf and Ms, in that the former decayed directly to the O intermediate whereas the latter decayed directly to BR.

Actinic light density dependence of the bacteriorhodopsin protocycle.

The photocycle of bacteriorhodopsin (BR) was studied in the 0.3 microsecond to 10 s time interval after excitation, using a wide range of actinic light intensities (10 ns half-duration, 0.06-60 mJ/cm2), at neutral and alkaline pH values. The relative weights of the rapidly and the slowly decaying components of the M intermediate (Mf and M(s), respectively) and the yield of the third millisecond component, N(R,P), are the function of the exciting light intensity (density), while their lifetimes are not. The relative weight of M(s) is found to be a linear function of the portion of the BR molecules undergoing the photocycle. This suggests the existence of a cooperative interaction of the BR molecules arranged in the crystalline purple membrane sheets. Another source of M(s) is also found, which results a nonvanishing relative weight of M(s) even at very weak actinic light density values. The explanation for this may be a branching, or the heterogeneity of BR itself or with its environment. It is shown that the relative weights of the rising and decaying components of the M form(s) do not correlate directly with each other.

Kinetics of the N intermediate and the two pathways of recovery of the ground-state of bacteriorhodopsin.

Absorption kinetic measurements at alkaline pH, in which bacteriorhodopsin (BR) is pre-excited by another flash, indicate that a part of the recovery of the BR ground-state is faster than the decay of the N intermediate of the photocycle. This fact proves the existence of a parallel pathway in the late part of the BR photocycle (the decay of Ms into BR), which does not include the N intermediate. We demonstrate that the decay of the Mf intermediate does not lead to any direct recovery of the BR ground-state, and that excitation of N does not form an M-like intermediate. Mf decays directly into the N intermediate, and photoexcitation of N leads to the formation of a red-shifted form, O*. The kinetics of this red-shifted intermediate are also presented.

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.

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.

Independent photocycles of the spectrally distinct forms of bacteriorhodopsin.

Time-resolved, flash-induced difference absorbance spectra (300-700 nm) at pH 10.5 and 5 degrees C for the bacteriorhodopsin photocycle fast and slow decaying forms of the M intermediate (M(f) and M(s), respectively) and R intermediate are reported. The main distinguishing features are as follows: For M(f), DeltaA(max) = 412 nm, a shoulder at 436 nm, no absorbance change at 350 nm; DeltaA(min) = 565 nm; DeltaA(412)/DeltaA(565) = 0.85. For M(s), DeltaA(max) = 412 nm, a shoulder at 386 nm; DeltaA(min) = 575 nm; DeltaA(412)/DeltaA(575) = 0.6. For R, DeltaA(max) = 336 and 350 nm (double peak), smaller peaks at 386 and 412 nm; DeltaA(min) = 585 nm; DeltaA(350)/DeltaA(585) = 0.2. The different difference spectra for M(f) and M(s) provide direct evidence that these species, initially identified by their kinetics, are physically distinct. With fast transient absorption spectroscopy, it was shown that R may form very fast, perhaps faster than the L intermediate decays. On the basis of the different bleaching peaks for M(f) and M(s), we propose that M(f) and M(s) are in independent photocycles formed from slightly different forms of bacteriorhodopsin. R may also be in a different photocycle. The different forms of bacteriorhodopsin are probably in dynamic equilibrium with their ratios, controlled by pH and temperature.

How Many M Forms are there in the Bacteriorhodopsin Photocycle?

On capturing a quantum of light, the bacteriorhodopsin of Halobacterium halobium undergoes a photocycle involving different intermediates. The exact scheme of the photocycle and especially the number of M intermediates are subjects of debate. For a quantitative analysis of many effects connected with the photocycle, e.g. the effect of the membrane potential on the kinetics of M decay (Groma et al., 1984. Biophys. J. 45:985-992), a knowledge of the exact photocycle is needed. In the present work sophisticated measurements were made on the decay kinetics of the M forms in cell envelope vesicles, purple membrane suspension and purple membrane fragments incorporated in polyacrylamide gel. The experimental data were analyzed by fitting one, two, and three discrete exponentials. Three different real components were found in the M decay of cell envelope vesicles in 4 M NaCl. All of them exhibited a temperature-dependence obeying the Arrhenius law. Two real components were found for the purple membrane in suspension and in gel in NaCl-free medium. The third phase appeared when the gel was soaked in 4 M NaCl. As an independent means of analysis, a continuous distribution of exponentials was also fitted to the M decay kinetics in cell envelope vesicles. This calculation also resulted in three processes with distinct rates or alternatively two processes with distributed rates.

Coupling between the bacteriorhodopsin photocycle and the protonmotive force in Halobacterium halobium cell envelope vesicles. II. Quantitation and preliminary modeling of the M----bR reactions.

The cell membrane of Halobacterium halobium (H. halobium) contains the proton-pump bacteriorhodopsin, which generates a light-driven transmembrane protonmotive force. The interaction of the bacteriorhodopsin photocycle with the electric potential component of the protonmotive force has been investigated. H. halobium cell envelope vesicles have been prepared by sonication and further purified by ultracentrifugation on Ficoll/NaCl/CsCl density gradients. Under continuous illumination (550 +/- 50 nm) varied from 0 to 40 mW cm-2, the vesicles maintain a membrane potential of 0 to -100 mV. The membrane potential was measured by flow dialysis of 3H-TPMP+ uptake and could be abolished by the uncoupler carbonylcyanide-m-chlorophenylhydrazone. Time-resolved absorption spectroscopy was used to measure the decay kinetics of the M photocycle intermediate, which was initiated by a weak laser flash (588 nm), while the vesicles were continuously illuminated as above. The M decay kinetics were fitted with two exponential decays by a computer deconvolution program. The faster decaying form decreases in amplitude (70 to 10% of the total) and the slower decaying form increases in amplitude and lifetime (23 to 42 ms) as the background light intensity increases. Although any correlation between the membrane potential and the bacteriorhodopsin photocycle M-forms is complex, the present data will allow specific tests of the physical mechanism for this interaction to be designed and conducted.

Electro-optical measurements on aqueous suspension of purple membrane from Halobacterium halobium.

The permanent dipole moment, polarizability, and the retinal angle of Halobacterium halobium purple membranes were determined at different pH values. All of the parameters have a maximum between pH 5 and 6. There is a reversal in the direction of the permanent dipole moment near pH 5. The value of permanent dipole moment was determined to be 60 D/protein at pH 6.6, and the value obtained for polarizability was 3 X 10(-28) Fm2/membrane fragment. The retinal angle of all-trans retinal was 0.8 degrees smaller than that of the 13-cis conformation.

The present state of the chemiosmotic coupling theory.

Although the general principles of the chemiosmotic coupling theory have become widely accepted, the (degree of) loc(aliz)ation of electrochemical proton potential difference cannot yet be deduced from the existing experimental data. Many results are not in ready accordance with the idea that one protonic electrochemical potential difference, i.e. the one between a homogeneous inner and a homogeneous outer aqueous phase, would be the high-free-energy intermediate of membrane-linked free-energy transduction. Rather, free-energy transduction in an organelle like a mitochondrion or a chloroplast might take place in large number (about 1 per H+-ATPase) of miniature chemiosmotic systems. The energized protons produced in such a miniature system might be largely (but not totally) confined to a proton-domain belonging to it. Hence, there might be many (rather than one) different relevant proton gradients.

Electric response of a back photoreaction in the bacteriorhodopsin photocycle.

The electric response of a back photoreaction in the bacteriorhodopsin photocycle was investigated. The proton pumping activity of green flash excited bacteriorhodopsin stops if the M412 form is illuminated by blue light (Karvaly and Dancsházy, 1977). In the present work a fast negative displacement current signal was measured in an oriented membrane suspension system, indicative of back movement of protons from M412 to BR570. Quantitative evaluation of the data shows that there are at least two steps in the back reaction, with different rate constants. The temperature dependence of the rate constants show simple linear Arrhenius behavior between 5 degree and 40 degree C. The rate constants were slower by a factor of 1.8 in D2O suspension. The relevance of the protein electric response signals (PERS) observed in this paper to the early receptor potential is discussed.

Investigation by focused laser beam scanning of the photoelectric activity of bacteriorhodopsin-containing lipid bilayers.

The photoelectric activity of different parts of lipid bilayer containing bacteriorhodopsin was investigated by moving a small actinic light spot across the Plateau-Gibbs border and the bimolecular part of this reconstituted model membrane. The results give direct evidence that bacteriorhodopsin incorporated into the bimolecular region of the lipid membrane is responsible for the photoelectric activity of this system. A technique for scanning the photoelectric activity of a modified bimolecular lipid membrane is described in detail.

Mechanism of generation and regulation of photopotential by bacteriorhodopsin in bimolecular lipid membrane.

Photoelectric properties of bacteriorhodopsin incorporated into a bimolecular lipid membrane were investigated with special regard to the mechanism of photoelectric field generation. It was shown that besides its proton pump and electric generator functions bacteriorhodopsin works as a possible molecular regulator of the light-induced membrane potential. When a bimolecular lipid membrane containing bacteriorhodopsin is continuously illuminated in its main visible absorption band, and afterwards by superimposed blue light matching the absorption band of the long-living photobleached bacteriorhodopsin (M412) as well, the latter either enhances or decreases the steady-state photoresponse, depending upon the intensity of the green light. Thus, the additional blue-light illumination tends to cause the resultant photoelectric membrane potential to become stabilized. Two alternative schemes are tentatively proposed for the photochemical cycle of bacteriorhodopsin whereby blue light can control photovoltage generation. A kinetic model of the proton pump and the regulation of the photoelectric membrane potential is presented. This model fits all the experimental findings, even quantitatively. From the model some kinetic and physical parameters of this light-driven pump could be determined.