[43] Resonance raman methods for proton translocation in bacteriorhodopsin

Low-temperature FTIR study of multiple K intermediates in the photocycles of bacteriorhodopsin and xanthorhodopsin

Low-temperature FTIR spectroscopy of bacteriorhodopsin and xanthorhodopsin was used to elucidate the number of K-like bathochromic states, their sequence, and their contributions to the photoequilibrium mixtures created by illumination at 80-180 K. We conclude that in bacteriorhodopsin the photocycle includes three distinct K-like states in the sequence bR (hv)--> I* --> J --> K(0) --> K(E) --> L --> ..., and similarly in xanthorhodopsin. K(0) is the main fraction in the mixture at 77 K that is formed from J. K(0) becomes thermally unstable above approximately 50 K in both proteins. At 77 K, both J-to-K(0) and K(0)-to-K(E) transitions occur and, contrarily to long-standing belief, cryogenic trapping at 77 K does not produce a pure K state but a mixture of the two states, K(0) and K(E), with contributions from K(E) of approximately 15 and approximately 10% in the two retinal proteins, respectively. Raising the temperature leads to increasing conversion of K(0) to K(E), and the two states coexist (without contamination from non-K-like states) in the 80-140 K range in bacteriorhodopsin, and in the 80-190 K range in xanthorhodopsin. Temperature perturbation experiments in these regions of coexistence revealed that, in spite of the observation of apparently stable mixtures of K(0) and K(E), the two states are not in thermally controlled equilibrium. The K(0)-to-K(E) transition is unidirectional, and the partial transformation to K(E) is due to distributed kinetics, which governs the photocycle dynamics at temperatures below approximately 245 K (Dioumaev and Lanyi, Biochemistry 2008, 47, 11125-11133). From spectral deconvolution, we conclude that the K(E) state, which is increasingly present at higher temperatures, is the same intermediate that is detected by time-resolved FTIR prior to its decay, on a time scale of hundreds of nanoseconds at ambient temperature (Dioumaev and Braiman, J. Phys. Chem. B 1997, 101, 1655-1662), into the K(L) state. We were unable to trap the latter separately from K(E) at low temperature, due to the slow distributed kinetics and the increasingly faster overlapping formation of the L state. Formation of the two consecutive K-like states in both proteins is accompanied by distortion of two different weakly bound water molecules: one in K(0), the other in K(E). The first, well-documented in bacteriorhodopsin at 77 K where K(0) dominates, was assigned to water 401 in bacteriorhodopsin. The other water molecule, whose participation has not been described previously, is disturbed on the next step of the photocycle, in K(E), in both proteins. In bacteriorhodopsin, the most likely candidate is water 407. However, unlike bacteriorhodopsin, the crystal structure of xanthorhodopsin lacks homologous weakly bound water molecules.

Two bathointermediates of the bacteriorhodopsin photocycle, from time-resolved nanosecond spectra in the visible

Time-resolved measurements were performed on wild-type bacteriorhodopsin with an optical multichannel analyzer in the spectral range 350-735 nm, from 100 ns to the photocycle completion, at four temperatures in the 5-30 degrees C range. The intent was to examine the possibility of two K-like bathochromic intermediates and to obtain their spectra and kinetics in the visible. The existence of a second K-like intermediate, termed KL, had been postulated (Shichida et al., Biochim. Biophys. Acta 1983, 723, 240-246) to reconcile inconsistencies in data in the pico- and microsecond time domains. However, introduction of KL led to a controversy, since neither its visible spectrum nor its kinetics could be confirmed. Infrared data (Dioumaev and Braiman, J. Phys. Chem. B 1997, 101, 1655-1662) revealed a state which might have been considered a homologue to KL, but it had a kinetic pattern different from that of the earlier proposed KL. Here, we characterize two distinct K-like intermediates, K(E) ("early") and K(L) ("late"), by their spectra and kinetics in the visible as revealed by global kinetic analysis. The K(E)-to-K(L) transition has a time constant of approximately 250 ns at 20 degrees C, and describes a shift from K(E) with lambda(max) at approximately 600 nm and extinction of approximately 56,000 M(-1) x cm(-1) to K(L) with lambda(max) at approximately 590 nm and extinction of approximately 50,000 M(-1) x cm(-1). The temperature dependence of this transition is characterized by an enthalpy of activation of DeltaH(++) approximately 40 kJ/mol and a positive entropy of activation of DeltaS(++)/R approximately 4. The consequences of multiple K-like states for interpreting the spectral evolution in the early stages of the photocycle are discussed.

Structural and mechanistic insight from high resolution structures of archaeal rhodopsins

Lipidic cubic phase-grown crystals yielded high resolution structures of a number of archaeal retinal proteins, the molecular mechanisms of which are being revealed as structures of photocycle intermediates become available. The structural basis for bacteriorhodopsin's mechanism of proton pumping is discussed, revealing a well-synchronized sequence of molecular events. Comparison with the high resolution structures of the halide pump halorhodopsin, as well as with the receptor sensory rhodopsin II, illustrates how small and localized structural changes result in functional divergence. Fundamental principles of energy transduction and sensory reception in the archaeal rhodopsins, which may have relevance to other systems, are discussed.

Deformation of Helix C in the Low Temperature L-intermediate of Bacteriorhodopsin

X-ray and electron diffraction studies of specific reaction intermediates, or reaction intermediate analogues, have produced a consistent picture of the structural mechanism of light-driven proton pumping by bacteriorhodopsin. Of central importance within this picture is the structure of the L-intermediate, which follows the retinal all-trans to 13-cis photoisomerization step of the K-intermediate and sets the stage for the primary proton transfer event from the positively charged Schiff base to the negatively charged Asp-85. Here we report the structural changes in bacteriorhodopsin following red light illumination at 150 K. Single crystal microspectrophotometry showed that only the L-intermediate is populated in three-dimensional crystals under these conditions. The experimental difference Fourier electron density map and refined crystallographic structure were consistent with those previously presented (Royant, A., Edman, K., Ursby, T., Pebay-Peyroula, E., Landau, E. M., and Neutze, R. (2000) Nature 406, 645-648; Royant, A., Edman, K., Ursby, T., Pebay-Peyroula, E., Landau, E. M., and Neutze, R. (2001) Photochem. Photobiol. 74, 794-804). Based on the refined crystallographic structures, molecular dynamic simulations were used to examine the influence of the conformational change of the protein that is associated with the K-to-L transition on retinal dynamics. Implications regarding the structural mechanism for proton pumping by bacteriorhodopsin are discussed.

Anion-protein interactions during halorhodopsin pumping: halide binding at the protonated Schiff base

Halorhodopsin (hR), the light-driven chloride pump of Halobacterium halobium, has been studied by Fourier transform infrared (FTIR) spectroscopy. Direct hydrogen bonding of halide ions with the protonated Schiff base (PSB) group was detected by means of halide-dependent perturbations on this group's vibrational frequencies. FTIR difference spectra were obtained of the hR-->hL photoreaction in reconstituted membrane vesicles. Nearly identical results were obtained using either low-temperature static difference spectroscopy at 1-cm-1 resolution or a stroboscopic time-resolved technique with 5-ms temporal and 2-cm-1 spectral resolution. The frequency of the negative difference band due to the PSB C = N stretch mode in the hR state shows a dependence on the type of halide counteranion that is present, 1632 cm-1 in the presence of Cl-, 1631 cm-1 in Br-, and 1629 cm-1 in I-. The C = NH+ stretch frequency thus correlates with the strength of the hydrogen bond formed by the halide. Analogous halide-dependent shifts of the C = NH+ frequency were observed in IR spectra of model compound retinylidene PSB salts. We also observed a significant halide dependence of the visible absorption maximum of hR solubilized in lauryl maltoside detergent. From such halide perturbation effects, we conclude that there is a direct hydrogen-bonded interaction between the Schiff base group and an externally supplied halide ion in the hR state. Halide perturbation effects are also observed for PSB-group vibrations in the hL state. Thus, despite an apparent overall weakening of hydrogen-bonding interactions of the PSB with its environment after chromophore photoisomerization to form hL, the PSB remains hydrogen-bonded to the halide. The results are best explained in terms of a "one-site, two-state" model for anion binding near the chromophore in the hR state, as opposed to a previously proposed two-site model.