Structural changes during the formation of early intermediates in the bacteriorhodopsin photocycle

Early intermediates of bacteriorhodopsin's photocycle were modeled by means of ab initio quantum mechanical/molecular mechanical and molecular dynamics simulations. The photoisomerization of the retinal chromophore and the formation of photoproducts corresponding to the early intermediates were simulated by molecular dynamics simulations. By means of the quantum mechanical/molecular mechanical method, the resulting structures were refined and the respective excitation energies were calculated. Two sequential intermediates were found with absorption maxima that exhibit red shifts from the resting state. The intermediates were therefore assigned to the K and KL states. In K, the conformation of the retinal chromophore is strongly deformed, and the N--H bond of the Schiff base points almost perpendicular to the membrane normal toward Asp-212. The strongly deformed conformation of the chromophore and weakened interaction of the Schiff base with the surrounding polar groups are the means by which the absorbed energy is stored. During the K-to-KL transition, the chromophore undergoes further conformational changes that result in the formation of a hydrogen bond between the N--H group of the Schiff base and Thr-89 as well as other rearrangements of the hydrogen-bond network in the vicinity of the Schiff base, which are suggested to play a key role in the proton transfer process in the later phase of the photocycle.     

Subpicosecond resonance Raman spectra of the early intermediates in the photocycle of bacteriorhodopsin

The resonance Raman spectra are presented for the species formed during the photocycle of bacteriorhodopsin (bR) on a timescale of 800-900 fs. In the ethylenic stretch region two intermediates were found with frequencies of 1,510 and 1,518 cm^-1, corresponding to species with optical absorption maxima at 660 and 625 nm, respectively. This leads to the assignment of the 1,518 cm^-1 band to the J₆₂₅ intermediate. In the fingerprint region, the appearance of a vibration at 1,195 cm^-1 strongly suggests that the isomerization indeed has taken place in a time less than the pulsewidth of our laser. This supports the previous proposals made on the basis of the optical spectra. The spectra are compared with those observed in tens of picoseconds up to nanoseconds.     

Molecular dynamics study of the 13-cis form (bR548) of bacteriorhodopsin and its photocycle.

The structure and the photocycle of bacteriorhodopsin (bR) containing 13-cis,15-syn retinal, so-called bR548, has been studied by means of molecular dynamics simulations performed on the complete protein. The simulated structure of bR548 was obtained through isomerization of in situ retinal around both its C13-C14 and its C15-N bond starting from the simulated structure of bR568 described previously, containing all-trans,15-anti retinal. After a 50-ps equilibration, the resulting structure of bR548 was examined by replacing retinal by analogues with modified beta-ionone rings and comparing with respective observations. The photocycle of bR548 was simulated by inducing a rapid 13-cis,15-anti-->all-trans,15-syn isomerization through a 1-ps application of a potential that destabilizes the 13-cis isomer. The simulation resulted in structures consistent with the J, K, and L intermediates observed in the photocycle of bR548. The results offer an explanation of why an unprotonated retinal Schiff base intermediate, i.e., an M state, is not formed in the bR548 photocycle. The Schiff base nitrogen after photoisomerization of bR548 points to the intracellular rather than to the extracellular site. The simulations suggest also that leakage from the bR548 to the bR568 cycle arises due to an initial 13-cis,15-anti-->all-trans,15-anti photoisomerization.     

Thermal equilibration between the M and N intermediates in the photocycle of bacteriorhodopsin.

The stages in the photocycle of bacteriorhodopsin (BR) involving the M and N intermediates are investigated using a double pulse excitation method. A first (cycling) pulse at 532 nm is followed, with an appropriate time delay, by a second pulse (337, 406, 446, or 470 nm) which induces the M-->BR back-photoreaction. After depletion by the second pulse a repopulation of M in the millisecond range is observed which is interpreted in terms of a thermal N-->M relaxation. It is thus concluded that a (thermal) M<-->N equilibrium accounts for the biphasic decay of M in the BR photocycle. Other models for this stage of the light-driven proton-pump are therefore unnecessary.     

Dynamics of primary events in the photocycle of excited bacteriorhodopsin

Transient dynamic behavior of the excited bacteriorhodopsin (BR), which was isolated from the strain H. salinarum, was studied at excitation wavelength from 585 to 639 nm. With the one-color femtosecond (fs) pump-probe technique, we revealed the primary events in BR's photocycle that took place in an ultrafast time scale. From the analysis of the decay components of the dynamical traces, it was evident that the isomerization of the retinal     

pH and salt effects on the slow intermediates of the bacteriorhodopsin photocycle

Purple membrane fragments of Halobacterium halobium were used to investigate pH and salt effects on the kinetics of M ₄₁₂, O ₆₆₀ and BR ₅₆₈. The flash-induced absorbance changes were measured in the 5–9 pH range, at low ionic strength and at 4 M NaCl. The results are consistent with a model which implies a branching in the last part of the bacteriorhodopsin photocycle.     

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.     

Protonation and deprotonation of the M, N, and O intermediates during the bacteriorhodopsin photocycle

Transient pH changes were measured with phenol red and chlorophenol red in the 30-microseconds-50-ms time range during the photocycle of bacteriorhodopsin (BR), the light-driven proton pump. At pH greater than or equal to 7, the results confirmed earlier data and suggestions that one proton is released during the L----M reaction, and taken up again during the decay of N. These are likely to be steps in the proton transport process. At pH less than 7, however, the time-resolved pH traces were complex and indicated additional protonation reactions. The data were explained by a model which assumed pH-dependent protonation states for M and N which varied from -1 to 0, and for O which varied from 0 to + 2, relative to BR. If the kinetics of the vectorial proton translocation process were taken as pH independent, this treatment of the data suggested that a residue with a pKa of 5.9 was made protonable in M and N and two residues with pKa's of 6.5 were made cooperatively protonable in O. The additional protons detected are not necessarily in the vectorial proton transfer pathway (i.e., they are probably "Bohr protons"), and while they must reflect conformational and/or neighboring ionization changes in the BR as it passes through the M, N, and O states, their role, if any, in the transport is uncertain.     

A time-resolved spectral study of the K and KL intermediates of bacteriorhodopsin.

Nanosecond time-resolved absorption measurements on the photolysis products of bacteriorhodopsin (BR) in intact membranes are reported. At room temperature in fluid solution a single intermediate (KL) is seen 10 ns after excitation. Both spectral and kinetic results are consistent with the KL intermediate converting to the L intermediate by a single first order reaction. The observed temperature-dependent rate has the Arrhenius parameters: Ea = 10.5 kcal/mol, A = 5 x 10(13) s-1. The precursor to the KL intermediate is also observed. Its spectral character is consistent with the K intermediate which has been previously reported. The current data is consistent with a linear sequence in the BR photocycle for K, KL, and L in room temperature fluid solution. Differences in the spectral characteristics of the K intermediates described here and elsewhere are discussed in terms of differences in the microenvironment around the retinal moiety and the affect this may have on the conformation of the chromophore.     

Late events in the photocycle of bacteriorhodopsin mutant L93A

In the photocycle of bacteriorhodopsin (bR) from Halobacterium salinarum mutant L93A, the O-intermediate accumulates and the cycling time is increased approximately 200 times. Nevertheless, under continuous illumination, the protein pumps protons at near wild-type rates. We excited the mutant L93A in purple membrane with single or triple laser flashes and quasicontinuous illumination, (i.e., light for a few seconds) and recorded proton release and uptake, electric signals, and absorbance changes. We found long-living, correlated, kinetic components in all three measurements, which-with exception of the absorbance changes-had not been seen in earlier investigations. At room temperature, the O-intermediate decays to bR in two transitions with rate constants of 350 and 1800 ms. Proton uptake from the cytoplasmic surface continues with similar kinetics until the bR state is reestablished. An analysis of the data from quasicontinuous illumination and multiple flash excitation led to the conclusion that acceleration of the photocycle in continuous light is due to excitation of the N-component in the fast N<-->O equilibrium, which is established at the beginning of the severe cycle slowdown. This conclusion was confirmed by an action spectrum.     

New photocycle intermediates in the photoactive yellow protein from Ectothiorhodospira halophila: picosecond transient absorption spectroscopy.

Previous studies have shown that the room temperature photocycle of the photoactive yellow protein (PYP) from Ectothiorhodospira halophila involves at least two intermediate species: I1, which forms in <10 ns and decays with a 200-micros lifetime to I2, which itself subsequently returns to the ground state with a 140-ms time constant at pH 7 (Genick et al. 1997. Biochemistry. 36:8-14). Picosecond transient absorption spectroscopy has been used here to reveal a photophysical relaxation process (stimulated emission) and photochemical intermediates in the PYP photocycle that have not been reported previously. The first new intermediate (I0) exhibits maximum absorption at approximately 510 nm and appears in </=3 ps after 452 nm excitation (5 ps pulse width) of PYP. Kinetic analysis shows that I0 decays with a 220 +/- 20 ps lifetime, forming another intermediate (Idouble dagger0) that has a similar difference wavelength maximum, but with lower absorptivity. Idouble dagger0 decays with a 3 +/- 0.15 ns time constant to form I1. Stimulated emission from an excited electronic state of PYP is observed both within the 4-6-ps cross-correlation times used in this work, and with a 16-ps delay for all probe wavelengths throughout the 426-525-nm region studied. These transient absorption and emission data provide a more detailed understanding of the mechanistic dynamics occurring during the PYP photocycle.     

Chromophore reorientations in the early photolysis intermediates of bacteriorhodopsin.

The photoselection-induced time-resolved linear dichroism of a bacteriorhodopsin suspension of purple membrane from 350 to 750 nm is measured by a new pseudo-null measurement technique. In combination with time-resolved absorption measurements, these linear dichroism measurements are used to determine the reorientation of the retinal chromophore of bacteriorhodopsin from 50 ns to 50 microseconds after photolysis. This time range covers the times when the K photointermediate decays to form L, as well as the early times during the formation of the M intermediate in the photocycle. An analysis of the photoselection-induced linear dichroism measured directly, along with the absorbance changes polarized parallel to the linearly polarized excitation, shows that the anisotropy is invariant over this time period, implying that the photolyzed chromophore rotates less than 8 degrees C with respect to unphotolyzed chromophores during this part of the photocycle.     

Nanosecond time-resolved infrared spectroscopy distinguishes two K species in the bacteriorhodopsin photocycle.

The photochemical reaction process of bacteriorhodopsin in the nanosecond time range (-120-860 ns) was measured in the 1400-900 cm-1 region with an improved time resolved dispersive-type infrared spectrometer. The system is equipped with a newly developed detection unit whose instrumental response to a 5-ns laser pulse has a full width of the half-maximum of 60 ns. It provides highly accurate data that enabled us to extract a kinetic process one order of magnitude faster than the instrumental response. The spectral changes in the 1400-900 cm-1 region were analyzed by singular value decomposition and resolved into three components. These components were separated by fitting with 10- and 1000-ns exponential functions and a step function, which were convoluted with the instrumental response function. The components with decay time constants of 10 and 1000 ns are named K and KL, respectively, on the basis of previous visible spectroscopy. The spectral shapes of K and KL are distinguishable by their hydrogen-out-of-plane (HOOP) modes, at 958 and 984 cm-1, respectively. The former corresponds to the K intermediate recorded at 77 K and the latter to a K-like photoproduct at 135 K. On the basis of published data, these bands are assigned to the 15-HOOP mode, indicating that the K and KL differ in a twist around the C14-C15 bond.     

Tyrosine and carboxyl protonation changes in the bacteriorhodopsin photocycle. 1. M412 and L550 intermediates

The role of tyrosines in the bacteriorhodopsin (bR) photocycle has been investigated by using Fourier transform infrared (FTIR) and UV difference spectroscopies. Tyrosine contributions to the BR570----M412 FTIR difference spectra recorded at several temperatures and pH's were identified by isotopically labelling tyrosine residues in bacteriorhodopsin. The frequencies and deuterium/hydrogen exchange sensitivities of these peaks and of peaks in spectra of model compounds in several environments suggest that at least two different tyrosine groups participate in the bR photocycle during the formation of M412. One group undergoes a tyrosinate----tyrosine conversion during the BR570----K630 transition. A second tyrosine group deprotonates between L550 and M412. Low-temperature UV difference spectra in the 220--350-nm region of both purple membrane suspensions and rehydrated films support these conclusions. The UV spectra also indicate perturbation(s) of one or more tryptophan group(s). Several carboxyl groups appear to undergo a series of protonation changes between BR570 and M412, as indicated by infrared absorption changes in the 1770--1720-cm-1 region. These results are consistent with the existence of a proton wire in bacteriorhodopsin that involves both tyrosine and carboxyl groups.     

Structure of an early intermediate in the M-state phase of the bacteriorhodopsin photocycle.

The structure of an early M-intermediate of the wild-type bacteriorhodopsin photocycle formed by actinic illumination at 230 K has been determined by x-ray crystallography to a resolution of 2.0 A. Three-dimensional crystals were trapped by illuminating with actinic light at 230 K, followed by quenching in liquid nitrogen. Amide I, amide II, and other infrared absorption bands, recorded from single bacteriorhodopsin crystals, confirm that the M-substate formed represents a structure that occurs early after deprotonation of the Schiff base. Rotation about the retinal C13-C14 double bond appears to be complete, but a relatively large torsion angle of 26 degrees is still seen for the C14-C15 bond. The intramolecular stress associated with the isomerization of retinal and the subsequent deprotonation of the Schiff base generates numerous small but experimentally measurable structural changes within the protein. Many of the residues that are displaced during the formation of the late M (M(N)) substate formed by three-dimensional crystals of the D96N mutant (Luecke et al., 1999b) are positioned, in early M, between their resting-state locations and the ones which they will adopt at the end of the M phase. The relatively small magnitude of atomic displacements observed in this intermediate, and the well-defined positions adopted by nearly all of the atoms in the structure, may make the formation of this structure favorable to model (simulate) by molecular dynamics.     

Molecular dynamics study of the M412 intermediate of bacteriorhodopsin.

Molecular dynamics simulations have been carried out to study the M412 intermediate of bacteriorhodopsin's (bR) photocycle. The simulations start from two simulated structures for the L550 intermediate of the photocycle, one involving a 13-cis retinal with strong torsions, the other a 13,14-dicis retinal, from which the M412 intermediate is initiated through proton transfer to Asp-85. The simulations are based on a refined structure of bR568 obtained through all-atom molecular dynamics simulations and placement of 16 waters inside the protein. The structures of the L550 intermediates were obtained through simulated photoisomerization and subsequent molecular dynamics, and simulated annealing. Our simulations reveal that the M412 intermediate actually comprises a series of conformations involving 1) a motion of retinal; 2) protein conformational changes; and 3) diffusion and reconfiguration of water in the space between the retinal Schiff base nitrogen and the Asp-96 side group. (1) turns the retinal Schiff base nitrogen from an early orientation toward Asp-85 to a late orientation toward Asp-96; (2) disconnects the hydrogen bond network between retinal and Asp-85 and tilts the helix F of bR, enlarging bR's cytoplasmic channel; (3) adds two water molecules to the three water molecules existing in the cytoplasmic channel at the bR568 stage and forms a proton conduction pathway. The conformational change (2) of the protein involves a 60 degrees bent of the cytoplasmic side of helix F and is induced through a break of a hydrogen bond between Tyr-185 and a water-side group complex in the counterion region.     

Nanosecond retinal structure changes in K-590 during the room-temperature bacteriorhodopsin photocycle: picosecond time-resolved coherent anti-stokes Raman spectroscopy.

Time-resolved vibrational spectra are used to elucidate the structural changes in the retinal chromophore within the K-590 intermediate that precedes the formation of the L-550 intermediate in the room-temperature (RT) bacteriorhodopsin (BR) photocycle. Measured by picosecond time-resolved coherent anti-Stokes Raman scattering (PTR/CARS), these vibrational data are recorded within the 750 cm-1 to 1720 cm-1 spectral region and with time delays of 50-260 ns after the RT/BR photocycle is optically initiated by pulsed (< 3 ps, 1.75 nJ) excitation. Although K-590 remains structurally unchanged throughout the 50-ps to 1-ns time interval, distinct structural changes do appear over the 1-ns to 260-ns period. Specifically, comparisons of the 50-ps PTR/CARS spectra with those recorded with time delays of 1 ns to 260 ns reveal 1) three types of changes in the hydrogen-out-of-plane (HOOP) region: the appearance of a strong, new feature at 984 cm-1; intensity decreases for the bands at 957 cm-1, 952 cm-1, and 939 cm-1; and small changes intensity and/or frequency of bands at 855 cm-1 and 805 cm-1; and 2) two types of changes in the C-C stretching region: the intensity increase in the band at 1196 cm-1 and small intensity changes and/or frequency shifts for bands at 1300 cm-1 and 1362 cm-1. No changes are observed in the C = C stretching region, and no bands assignable to the Schiff base stretching mode (C = NH+) mode are found in any of the PTR/CARS spectra assignable to K-590. These PTR/CARS data are used, together with vibrational mode assignments derived from previous work, to characterize the retinal structural changes in K-590 as it evolves from its 3.5-ps formation (ps/K-590) through the nanosecond time regime (ns/K-590) that precedes the formation of L-550. The PTR/CARS data suggest that changes in the torsional modes near the C14-C15 = N bonds are directly associated with the appearance of ns/K-590, and perhaps with the KL intermediate proposed in earlier studies. These vibrational data can be primarily interpreted in terms of the degree of twisting of the C14-C15 retinal bond. Such twisting may be accompanied by changes in the adjacent protein. Other smaller, but nonetheless clear, spectral changes indicate that alterations along the retinal polyene chain also occur. The changes in the retinal structure are preliminary to the deprotonation of the Schiff base nitrogen during the formation of M-412. The time constant for the ps/ns K-590 transformation is estimated from the amplitude change of four vibrational bands in the HOOP region to be 40-70 ns.     

Chromophore motion during the bacteriorhodopsin photocycle: polarized absorption spectroscopy of bacteriorhodopsin and its M-state in bacteriorhodopsin crystals.

The three-dimensional crystallization of bacteriorhodopsin was systematically investigated and the needle-shaped crystal form analysed. In these crystals the M-intermediate forms 10 times faster and decays 15 times more slowly than in purple membranes. Polarized absorption spectra of the crystals were measured in the dark and light adapted states. A slight decrease in the angle between the transition moment and the membrane plane was detected during dark adaptation. The crystallization of a mutated bacteriorhodopsin, in which the aspartic acid at residue 96 was replaced by asparagine, provided crystals with a long lived M-intermediate. This allowed polarized absorption measurements of the M-chromophore. The change in the polarization ratio upon formation of the M-intermediate indicates an increase in the angle between the main transition dipole and the membrane plane by 2.2 degrees +/- 0.5, corresponding to a 0.5 A displacement of one end of the chromophore out of the membrane plane of the bacteriorhodopsin molecule.     

The bacteriorhodopsin photocycle: direct structural study of two substrates of the M-intermediate.

Changes in protein structure that occur during the formation of the M photointermediate of bacteriorhodopsin can be directly visualized by electron diffraction techniques. A modified preparation technique for glucose-embedded crystals was employed to ensure sufficient hydration of the crystals, which was needed for the formation of the M intermediate at low temperature. Samples containing a high percentage of the M intermediate were trapped by rapidly cooling the crystals with liquid nitrogen after illumination with filtered green light at 240 and 260 K, respectively. Difference Fourier projection maps are presented for the M intermediates formed at these two temperatures. The diffraction data clearly show that statistically significant structural changes occur upon formation of the M intermediate at 240 K and then further upon formation of the second specimen that is produced at 260 K.     

Pathways of proton release in the bacteriorhodopsin photocycle.

The pH dependencies of the rate constants in the photocycles of recombinant D96N and D115N/D96N bacteriorhodopsins were determined from time-resolved difference spectra between 70 ns and 420 ms after photoexcitation. The results were consistent with the model suggested earlier for proteins containing D96N substitution: BR hv----K----L----M1----M2----BR. Only the M2----M1 back-reaction was pH-dependent: its rate increased with increasing [H+] between pH 5 and 8. We conclude from quantitative analysis of this pH dependency that its reverse, the M1----M2 reaction, is linked to the release of a proton from a group with a pKa = 5.8. This suggests a model for wild-type bacteriorhodopsin in which at pH greater than 5.8 the transported proton is released on the extracellular side from this as yet unknown group and on the 100-microseconds time scale, but at pH less than 5.8, the proton release occurs from another residue and later in the photocycle most likely directly from D85 during the O----BR reaction. We postulate, on the other hand, that proton uptake on the cytoplasmic side will be by D96 and during the N----O reaction regardless of pH. The proton kinetics as measured with indicator dyes confirmed the unique prediction of this model: at pH greater than 6, proton release preceded proton uptake, but at pH less than 6, the release was delayed until after the uptake. The results indicated further that the overall M1----M2 reaction includes a second kinetic step in addition to proton release; this is probably the earlier postulated extracellular-to-cytoplasmic reorientation switch in the proton pump.