A DETAILED RESONANCE RAMAN STUDY OF THE M412 INTERMEDIATE IN THE BACTERIORHODOPSIN PHOTOCYCLE

Abstract— Resonance Raman spectra of various M₄₁₂ species associated with the bacteriorhodopsin photocycle have been obtained. These correspond to the two forms observed during the formation of M₄1₂ and the two forms that are observed during its decay in absorption experimeents. We do not see any significant difference between the Raman spectra of any of these forms. We therefore conclude that the differences in these species are due to the differences in the protein structure and not in the chromophore.     

RESONANCE RAMAN STUDIES OF BACTERIORHODOPSIN ANALOGUES

Abstract— We present the results of resonance Raman measurements on a series of bacteriorhodopsin (bR) analogues formed from synthetic retinals which have replaced the native chromophore in the active site. Specifically, 5,6-dihydro-bR, 13-desmethyl-bR, 10-methyl-bR, 14-methyl-bR, and 10.14-dimethyl-bR have been studied. All five analogues bind and form Schiff base retinal-apoprotein linkages. While the Schiff base linkages of 5,6-dihydro-bR, 13-desmethyl-bR, and 10-methyl-bR are protonated, like the native chromophore, the 14-methyl-bR, and 10,14-dimethyl-bR Schiff bases are unprotonated. These results suggest that the binding site of bacteriorhodopsin near the Schiff base moiety is different from that of rhodopsin. The protonated Schiff base -C=NH- stretching frequency of 5.6-dihydro-bR lies at 1660 cm^-1 which is unusually high for a bacteriorhodopsin based pigment. The downward shift upon deuteration is 16 cm^-1, essentially identical to that measured for bacteriorhodopsin. This and the other analogue results strongly reinforce our previous arguments that the Schiff base stretching frequency is determined in large part by two factors, the C=N force constant and the stretch interaction with C=N-H bend. On the other hand, the deuterium isotope effect is determined primarily by the stretch-bend interaction.     

ULTRAVIOLET RESONANCE RAMAN SPECTROSCOPY OF BACTERIORHODOPSIN

Ultraviolet resonance Raman spectra of bacteriorhodopsin have been obtained using 229 nm excitation from a hydrogen-shifted neodymium yttrium aluminum garnet (Nd: YAG) laser. High signal-to-noise spectra are observed exhibiting vibrational bands at 762, 877, 1011, 1175, 1356, 1552 and 1617 cm-1 which are assigned to scattering from tryptophan and tyrosine side chains. This demonstrates the feasibility of using UV resonance Raman spectroscopy to monitor aromatic amino acid structural changes during the bacteriorhodopsin photocycle.     

TIME-RESOLVED RESONANCE RAMAN STUDIES ON THE PHOTOCHEMICAL CYCLE OF BACTERIORHODOPSIN

Abstract— Kinetic resonance Raman (RR) experiments were designed to study the time-behaviour of the retinal-binding protein bacteriorhodopsin (BR) in its photochemical cycle. The unphotolyzed chro-mophore B-570 and the two intermediates L -550 and M-412 were probed by the characteristic C=C stretching vibrations of the retinal moiety. Time resolution was achieved with a spinning cell as flow system in combination with two CW lasers in a pump-probe configuration. RR spectra were probed at 475 nm at various delay times between pump and probe event. The deconvolution of the spectra into the various components B-570, L-550 and M-412 was carried out by curve fitting procedures. It was found that at pH7.4 L-550 decays — with a time-constant of 62 μs — not completely but to a residual level of 35% of its initial value. This intermediate L -amplitude finally disappears in the ms-range (4.5 ms) synchroneously with the intermediate M -412. An analogeous time-behaviour was found at pH 4.6. In the basic range also an " L " -intermediate could be identified which is coupled to the long-lived M-component. To explain the peculiar time-dependence it is proposed that during the fast decay of L a dynamic equilibrium between L and M is established. Then during the reconstitution of B -570 the two intermediates disappear synchroneously. A molecular model is presented in which the dynamic equilibrium between L and M is explained by an oscillatory motion of a proton from the Schiff base group of the chromophore to its counterion.     

TIME-RESOLVED RESONANCE RAMAN SPECTRA OF THE PHOTOCYCLE INTERMEDIATES OF ACID AND DEIONIZED BACTERIORHODOPSIN

Abstract— The photocycle of bacteriorhodopsin (bR) and its perturbed forms are investigated by a time-resolved resonance Raman study. These experiments were performed in the C=C stretching and in the fingerprint spectral regions for the acid blue, acid purple and deionized forms of bR.
The main observations are as follows: (1) isomerization of the retinal, from all- trans to 13- cis , occurs in native bR and in all of the acid and deionized perturbed bR species; (2) formation of the early intermediates (the K₆₁₀ and L₅₅₀ analogues) also occur in native bR and in all of the perturbed species; and (3) deprotonation of the protonated Schiff base (PSB), to give the M₄₁₂ type intermediate, occurs in native bR, but is inhibited in all of the perturbed bR species on the time-scale of the native bR photocycle.
The results show that isomerization alone is not a prerequisite for the PSB deprotonation process. The observed photocycle, initiated with retinal isomerization, is found to occur from all- trans to 13- cis in all of the perturbed forms of bR. In addition, the results imply that removal of the cations, of an increase in the hydrogen ion concentration, prevent only the PSB deprotonation process and not the formation of earlier cycle intermediates. Some attention is focused on the two blue forms of bR (acid and deionized) due to the fact that their ground-state absorption maximum, unphotolyzed Raman spectra, and Raman spectra changes during the photocycle are all very similar. The similarities between the acid blue and deionized blue forms in the fingerprint region support previous suggestions that both blue species have nearly the same retinal active site.     

TIME-RESOLVED RESONANCE RAMAN SPECTROSCOPY OF THE BACTERIORHODOPSIN PHOTOCYCLE ON THE PICOSECOND AND NANOSECOND TIME SCALES

Abstract— Resonance Raman spectra of the picosecond bacteriorhodopsin intermediate(s) have been obtained by microbeam, flow and subtraction techniques using a synchronously pumped, cavity-dumped dye laser. Nanosecond spectra also were measured with this laser by cavity dumping without mode-locking. The picosecond spectra in the fingerprint region, which is sensitive to the configuration of the retinal chromophore, differ from spectra of the parent bR₅₇₀ but could be correlated to the spectrum of bR^DA₅₅₀ , a “13-cis” species which has been determined from spectra of bR₅₇₀ and bR^DA₅₆₀. The picosecond transient and bR^DA₅₅₀ also are similar in the 950–1050 cm^-1“deuteration fingerprint” region when the medium is changed from H₂O to D₂O. These results suggest that trans—cis isomerization occurs during the 40-ps pulse duration. The shift relative to the parent bR₅₇₀ in the ethylenic stretch region suggests that the picosecond and nanosecond transients absorb at wavelengths longer than 570 nm. The C band at 1646 cm^-1 is found to shift or to broaden upon photolysis in the picosecond time scale. This might suggest a change in the electronic structure of the group and its environment on the picosecond time domain. The nanosecond spectra obtained in this work (with 15-ns pulses) are similar to the spectra previously observed on the 100-ns time scale but are slightly different from the picosecond spectrum. These data suggest that more than one transient species appears on the picosecond-to-nanosecond time scale. The temporal evolution of Raman bands in the fingerprint as well as the low energy (950–1050 cm^-1) region and its implications are discussed.     

ON THE TWO FORMS OF INTERMEDIATE M OF BACTERIORHODOPSIN

Abstract— The decay time course of intermediate M of bacteriorhodopsin was investigated by flash spectrophotometry. The decay was composed of two exponentials showing the existence of two forms of intermediate absorbing around 410 nm. The two were very different in kinetic character whereas the absorption spectra were almost the same. The relative yield of the two components was a function of the intensity of the exciting flash and the slower component disappeared when the flash intensity was made very small. A model based on the trimeric cluster structure of bacteriorhodopsin is proposed.     

RESONANCE RAMAN AND SURFACE-ENHANCED RESONANCE RAMAN SPECTROSCOPY OF HYPERICIN

Hypericin has been found to exhibit a variety of photodynamic effects. To correlate biological activity with molecular structure, complete physical characterization of hypericin is required. The vibrational spectrum has been determined and resonance Raman and surface enhanced resonance Raman scattering spectra are reported. In addition, the Raman spectrum of a model compound has been studied to facilitate assignment of the vibrational modes of hypericin.     

POWER- AND TIME-RESOLVED RESONANCE RAMAN STUDIES AND CONFORMATIONAL CHANGES IN BACTERIORHODOPSIN

Abstract— By comparing the resonance Raman spectra of the retinal of the intermediates of bacteriorho-dopsin (obtained by using fixed flow with residence of time of 10 ps. variable laser power and frequency as well as computer subtraction techniques) with those of model compounds and with each other, the following possible conclusions can be obtained: (1) There exists stronger interaction between the retinal and the opsin in bacteriorhodopsin than that present in rhodopsin. (2) Conformational changes seem to take place during the dark light adaptation process as well as during the photosynthetic cycle. (3) The appearance of the spectrum of the retinal in the fingerprint region for the bL₅₅₀ and bM₄₁₂ intermediates is similar despite large shifts in their optical absorption maxima. This might argue against the theory that proposes ground state retinal conformational changes to explain the observed red shift in the optical spectra of retinal upon combining with the opsin. (4) Contrary to bM ₄₁₂ , the bL₅₅₀ species seems to be protonated. The fact that loss of proton does not seem to change the retinal conformation greatly might suggest that the protein and its ionic environment might carry the larger share of the load in the deprotonation process.     

PRIMARY PHOTOCHEMISTRY OF BACTERIORHODOPSIN: COMPARISON OF FOURIER TRANSFORM INFRARED DIFFERENCE SPECTRA WITH RESONANCE RAMAN SPECTRA

Abstract —Fourier transform infrared (FTIR) difference spectra of the BR→rK transition in bacteriorhodopsin at 77→K are compared with analogous resonance Raman difference spectra obtained using a spinning sample cell at 77→K. The vibrational frequencies observed in the FTIR spectra of native purple membrane and of purple membrane regenerated with 15-deuterioretinal are in good agreement with the frequencies observed in the Raman spectra, indicating that the lines in the FTIR difference spectra arise predominantly from retinal chromophore vibrations. This agreement confirms that the spinning cell method for obtaining resonance Raman spectra of K minimizes potential contributions from unwanted photoproducts. The unexpected similarity between the resonance Raman scattering intensities and the FTIR absorption intensities for BR and K is discussed in terms of the delocalized electronic structure of the chromophore. Finally, comparison of the Schiff base regions of the K Raman and FTIR spectra provide additional information on the assignment of its Schiff base vibration.     

掺杂态聚苯胺的共振拉曼光谱研究

观测了聚苯胺(PAn)在不同状态(掺杂、反掺杂、碱式、氧化、还原)下的拉曼光谱.根据其光谱特性,结合其它实验结果,提出了掺杂态PAn分子链包含电荷分布不等的三种苦环和二种氮原子的四单元苯醌变体模型,指出质子酸掺杂系分子内氧化还原反应,讨论了PAn氧化程度对掺杂效率的影响.     

RESONANCE RAMAN SPECTRA OF BACTERIORHODOPSIN MUTANTS WITH SUBSTITUTIONS AT ASP-85, ASP-96, AND ARG-82

Detergent solubilized bacteriorhodopsin (BR) proteins which contain alterations made by site-directed mutagenesis (Asp-96----Asn, D96N; Asp-85----Asn, D85N; and Arg-82----Gln, R82Q) have been studied with resonance Raman spectroscopy. Raman spectra of the light-adapted (BRLA) and M species in D96N are identical to those of native BR, indicating that this residue is not located near the chromophore. The BRLA states of D85N and especially R82Q contain more of the 13-cis, C = N syn (BR555) species under ambient illumination compared to solubilized native BR. Replacement of Asp-85 with Asn causes a 25 nm red-shift of the absorption maximum and a frequency decrease in both the ethylenic (-7 cm-1) and the Schiff base C = NH+ (-3 cm-1) stretching modes of BRLA. These changes indicate that Asp-85 is located close to the protonated retinal Schiff base. The BRLA spectrum of R82Q exhibits a slight perturbation of the C = NH+ band, but its M spectrum is unperturbed. The Raman spectra and the absorption properties of D85N and R82Q suggest that the protein counterion environment involves the residues Asp-85-, Arg-82+ and presumably Asp-212-. These data are consistent with a model where the strength of the protein-chromophore interaction and hence the absorption maximum depends on the overall charge of the Schiff base counterion environment.     

QUANTUM YIELD RATIO OF THE FORWARD and BACK LIGHT REACTIONS OF BACTERIORHODOPSIN T LOW TEMPERATURE and PHOTOSTEADY-STATE CONCENTRATION OF THE BATHOPRODUCT K*

The maximum photosteady state fraction of K, x_K^max, and the ratio of the quantum yields of the forward and back light reactions, trans-bacteriorhodopsin (bR) hArr; K, φ_bR/φ_K, were obtained by measuring the absorption changes produced by illumination of frozen water-glycerol (1:2) suspensions of light-adapted purple membrane at different wavelengths at -165°C. An independent method based on the second derivative of the absorption spectrum in the region of the β-bands was also used. It was found that The quantum yield ratio (0.66 ± 0.06) was found to be independent of excitation wavelength within experimental error in the range510–610 nm. The calculated absorption spectrum of K has its maximum at603–606 nm and an extinction 0.85 ± 0.03 that of bR. At shorter wavelengths there are P-bands at 410, 354 and 336 rim. Using the data of Hurley et al. (Nature 270,540–542, 1977) on relative rates of rhodopsin bleaching and K formation, the quantum yield of K formation was determined to be 0.66 ± 0.04 at low temperature. The quantum efficiency of the back reaction was estimated to be 0.93 ± 0.07. These values of quantum efficiencies of the forward and back light reactions of bR at - 165°C coincide with those recently obtained at room temperature. This indicates that the quantum efficiencies of both forward and back light reactions of bacteriorhodopsin are temperature independent down to -165°C.     

ULTRAVIOLET RESONANCE RAMAN STUDY ON PURPLE AND BLUE MEMBRANES OF Halobacterium halobium

Abstract— Two hundred and forty and 213 nm excited resonance Raman spectra of purple membrane (PM) and blue membrane (BM) of Halobacterium halobiurn were studied. Generally intense Trp scattering and a strong relative intensity of the W3 band at 1553 cm^-1 in the 240 nm spectrum of PM indicate red-shifted B_b absorptions of some Trp sidechains. A high intensity ratio of Trp doublet at 1360 and 1340 cm^-1 suggests interactions with highly hydrophobic Trp environments. These Trp are not strongly H-bonded and their N₁ sites are located in positions easily reached by solvent water molecules. Tyrosines are also in very hydrophobic environments and H-bonded. The mainchain consists of normal and distorted α-helices whose amide NH are hardly deuterated in D₂O suspension, and some NH exchangeable irregular segments on the membrane surface. Upon acidification, the ratio of Trp doublet with 240 nm excitation decreases concomitant with increase in retinal absorbance at 600 nm, and the W3 relative intensity and overall Trp scattering also decrease. These observations strongly indicate that the counterpart of Trp interactions in PM is the retinal and that the interactions partly diminish upon acidification. The Tyr environment also changes with the color. Although the 240 nm amide I intensity is greater in acid BM than in PM, the change is not related to the color change because the amide I intensity of deionized BM is practically the same as that of PM. The amide I intensity increase in acid BM is ascribable to a structural change of the surface peptides due to acid induced aggregation.     

RESONANCE RAMAN SPECTRA OF THE Pr-FORM OF PHYTOCHROME

Abstract— Resonance Raman spectra of the P_r-form of oat phytochrome have been obtained at 77 K. Interference from phytochrome fluorescence is avoided by employing far-red 752 nm excitation. Vibrational assignments are suggested for the tetrapyrrole chromophore in phytochrome by comparison with previously published model compound spectra and by examining the characteristic shifts induced by deuteration of the pyrrole nitrogens. The lack of carbonyl intensity, the frequencies of the 1626 and 1644 cm^-1 C=C stretching modes, and the presence of an intense mode at 1326 cm^-1 are all consistent with a protonated structure for the tetrapyrrole chromophore in P_r. This suggests that the -50 nm red-shift of the protein-bound chromophore absorption compared to the chromophore in vitro is caused by protonation of the pyrrole nitrogen.     

QUANTUM EFFICIENCY FOR THE PHOTOCONVERSION OF BACTERIORHODOPSIN AT VERY LOW TEMPERATURES

Abstract— Quantum efficiencies for photoconversion of bacteriorhodopsin (trans-bR) to a bathochromic product (batho-bR^t) and its photoreversion in purple membrane at 77 and 9 K were investigated with low temperature spectrophotometry. The kinetics of the photoconversion and its photoreversion cannot be expressed by a single exponential curve. The photoconversions at 77 and 9 K showed the same slope in the early stage. The kinetics of the photoreversions were identical at the two temperatures. These results indicate that the quantum efficiencies for the conversion of trans-bR to batho-bR^t or for its photoreversion are identical at the two temperatures.
The fact that the photoreversion cannot be expressed by a single exponential curve suggests the existence of several conformational states of batho-bR^t due to the trimer structure of the purple membrane.     

EVIDENCE FOR BRANCHING IN THE PHOTOCYCLE OF BACTERIORHODOPSIN AND CONCENTRATION CHANGES OF LATE INTERMEDIATE FORMS

Abstract— Flash photolysis transients of bacteriorhodopsin were recorded with a spectrograph -multielement photodiode array combination and the recordings were analyzed to determine the concentrations of bacteriorhodopsin intermediates "M" and "O" relative to the amount of "bR" cycling (pH 7.1,10–40°C). Estimated concentration time courses were simulated with solutions to two kinetic decay models which could account for photocycle temperature dependence. A unidirectional unbranched decay model overpredicts our estimated levels of [O(r)], whereas a model branched at the "M" intermediate describes each of the later intermediate levels well (with no evidence for an independent "N" form). Our results are consistent with "M" decay regulating the level and rates of change of [bR (t)] and (bR(f)]- and also suggest that two temperature-dependent pathways form "bR" from "M", one directly, and the other indirectly through "O".     

RESONANCE RAMAN SPECTRUM OF THE EXCITED 21Ag STATE OF ß-CAROTENE

Abstract— Resonance Raman (RR) bands assignable to the 2¹A_g excited state of ß-carotene are recorded using picosecond time-resolved resonance Raman (PTR³) spectroscopy. The RR spectrum contains bands in both the C-C (1204 cm^?1, 1243 cm^?1, and 1282 cm^?1) and C=C (1777 cm^?1) stretching regions. The time-dependent intensities of these RR features, measured with ? 30 ps. resolution, are found (i) to closely correlate with picosecond transient absorption (PTA) data recorded at 575 nm on the same sample and (ii) inversely correlate with the time-dependent intensities of RR bands assigned to the 1¹A_g ground state. Both of these observations support the assignment of these four RR features to the 2¹A_g excited state. These results remove uncertainties associated with earlier experiments in which excited-state RR scattering from (3-carotene was not observed in spite of predicted trends emanating from studies of shorter polyene compounds. The observed C=C band position also agrees with a recent report of this feature.     

PHYTOCHROME INTERMEDIATES IN VIVO– III KINETIC ANALYSIS OF INTERMEDIATE REACTIONS AT LOW TEMPERATURE

Abstract— Kinetic experiments have provided evidence for a series of light and dark reactions of phytochrome intermediates at low temperature in Pisum epicotyl tissue. A photoequilibrium exists between P_r and P₆₉₈, and between P_fr and P₆₅₀. A dark reversion of P₆₉₈P_r and P₆₅₀p_fr at –70°C has been demonstrated. When cooled to 70°C under incandescent light, most of the phytochrome in the tissue is driven into photochemically unreactive intermediates. About 2% of the phytochrome remains as weakly absorbing intermediates that form P_r and P_fr in darkness. A scheme is presented for phytochrome phototransformation in vivo.     

THE ORIGIN OF THE RED-SHIFTED ABSORPTION MAXIMUM OF THE M412 INTERMEDIATE IN THE BACTERIORHODOPSIN PHOTOCYCLE

The factors that red shift the absorption maximum of the retinal Schiff base chromophore in the M₄₁₂ intermediate of bacteriorhodopsin photocycle relative to absorption in solution were investigated using a series of artificial pigments and studies of model compounds in solution. The artificial pigments derived from retinal analogs that perturb chromophore-protein interactions in the vicinity of the ring moiety indicate that a considerable part of the red shift may originate from interactions in the vicinity of the Schiff base linkage. Studies with model compounds revealed that hydrogen bonding to the Schiff base moiety can significantly red shift the absorption maximum. Furthermore, it was demonstrated that although s-trans ring-chain planarity prevails in the M₄₁₂ intermediate it does not contribute significantly (only ca 750 cm⁻¹) to the opsin shift observed in M₄₁₂. It is suggested that in M₄₁₂, the Schiff base linkage is hydrogen bonded to bound water and/or protein residues inducing a considerable red shift in the absorption maximum of the retinal chromophore.