Structure of the retinal chromophore in the hRL intermediate of halorhodopsin from resonance raman spectroscopy

Time-resolved resonance Raman spectra of the hRL intermediate of halorhodopsin have been obtained. The structurally sensitive fingerprint region of the hRL spectrum is very similar to that of bacteriorhodopsin's L550 intermediate, which is known to have a 13-cis configuration. This indicates that hRL contains a 13-cis chromophore and that an all-trans----13-cis isomerization occurs in the halorhodopsin photocycle. hRL exhibits a Schiff base stretching mode at 1644 cm-1, which shifts to 1620 cm-1 in D2O. This demonstrates that the Schiff base linkage to the protein is protonated. The insensitivity of the C-C stretching mode frequencies to N-deuteriation suggests that the Schiff base configuration is anti. The 24 cm-1 shift of the Schiff base mode in D2O indicates that the Schiff base proton in hRL has a stronger hydrogen-bonding interaction with the protein than does hR578.     

Structure of the retinal chromophore in sensory rhodopsin I from resonance Raman spectroscopy

Sensory rhodopsin I (SR-I) is a retinal-containing pigment which functions as a phototaxis receptor in Halobacterium halobium. We have obtained resonance Raman vibrational spectra of the native membrane-bound form of SR587 and used these data to determine the structure of its retinal prosthetic group. The similar frequencies and intensities of the skeletal fingerprint modes in SR587, bacteriorhodopsin (BR568), and halorhodopsin (HR578) as well as the position of the dideuterio rocking mode when SR-I is regenerated with 12,14-D2 retinal (915 cm-1) demonstrate that the retinal chromophore has an all-trans configuration. The shift of the C = N stretching mode from 1628 cm-1 in H2O to 1620 cm-1 in D2O demonstrates that the chromophore in SR587 is bound to the protein by a protonated Schiff base linkage. The small shift of the 1195 cm-1 C14-C15 stretching mode in D2O establishes that the protonated Schiff base bond has an anti configuration. The low value of the Schiff base stretching frequency together with its small 8 cm-1 shift in D2O indicates that the Schiff base proton is weakly hydrogen bonded to its protein counterion. This suggests that the red shift in the absorption maximum of SR-I (587 nm) compared with HR (578 nm) and BR (568 nm) is due to a reduction of the electrostatic interaction between the protonated Schiff base group and its protein counterion.     

Conformational changes in sensory rhodopsin I: similarities and differences with bacteriorhodopsin, halorhodopsin, and rhodopsin

FTIR difference spectra have been obtained for the sR587----S373 phototransition of sensory rhodopsin I (sR-I), a signal-transducing protein of Halobacterium halobium. The vibrational modes of the sR587 chromophore have frequencies close to those of the bacteriorhodopsin bR568 chromophore, confirming that the two chromophores have very similar structures and environments. However, the sR-I Schiff base C = N stretch frequency is downshifted relative to bR, consistent with weaker hydrogen bonding with its counterion(s). The carboxyl (COOH) stretch modes of sR-I and halorhodopsin (hR) are at the same frequencies. On the basis of sequence homologies, these bands can be assigned to Asp-106 in helix D and/or Asp-201 in helix G. In contrast, no band was found that could be assigned to the protonation of Asp-76. In bR, the homologous residue Asp-85 serves as the acceptor group for the Schiff base proton. Bands appear in the amide I and II regions at similar frequencies in sR-I, hR, and bR, indicating that despite their different functions they all undergo closely related structural changes. Bands are also detected in the C-H stretch region, possibly due to alterations in the membrane lipids. Similar spectral features are also observed in the lipids of rhodopsin-containing photoreceptor membrane upon light activation.     

Chloride ion binding to bacteriorhodopsin at low pH: an infrared spectroscopic study

Bacteriorhodopsin (bR) and halorhodopsin (hR) are light-induced ion pumps in the cell membrane of Halobacterium salinarium. Under normal conditions bR is an outward proton transporter, whereas hR is an inward Cl- transporter. There is strong evidence that at very low pH and in the presence of Cl-, bR transports Cl- ions into the cell, similarly to hR. The chloride pumping activity of bR is connected to the so-called acid purple state. To account for the observed effects in bR a tentative complex counterion was suggested for the protonated Schiff base of the retinal chromophore. It would consist of three charged residues: Asp-85, Asp-212, and Arg-82. This quadruplet (including the Schiff base) would also serve as a Cl- binding site at low pH. We used Fourier transform infrared difference spectroscopy to study the structural changes during the transitions between the normal, acid blue, and acid purple states. Asp-85 and Asp-212 were shown to participate in the transitions. During the normal-to-acid blue transition, Asp-85 protonates. When the pH is further lowered in the presence of Cl-, Cl- binds and Asp-212 also protonates. The binding of Cl- and the protonation of Asp-212 occur simultaneously, but take place only when Asp-85 is already protonated. It is suggested that HCl is taken up in undissociated form in exchange for a neutral water molecule.     

Resonance Raman study of halorhodopsin photocycle kinetics, chromophore structure, and chloride-pumping mechanism.

Kinetic resonance Raman spectra of the HR520, HR640, and HR578 species in the halorhodopsin photocycle are obtained using time delays ranging from 5 microseconds to 10 ms in 0.3 M NO3-, 0.3 M Cl-, and 3 M Cl-. The Raman intensities are converted to absolute concentrations by using a conservation of molecules constraint. The simplest kinetic scheme that satisfactorily models the data is HR578-->HR520 in equilibrium with HR640-->HR578. The rate constant for the HR640-->HR578 transition increases with Cl- concentration, suggesting that Cl- is taken up between HR640 and HR578. The ratio of the forward to the reverse rate constants connecting HR520 and HR640 increases as the inverse of the Cl- concentration, suggesting that Cl- is released during the HR520-->HR640 step. The configuration about the C13 = C14 bond of the retinal chromophore in HR640 is examined by regenerating the protein with [12,14-2H2]retinal. The C12-2H + C14-2H rocking vibration for HR640 is observed at 943 cm-1, demonstrating that the chromophore is 13-cis. The changes in the resonance Raman spectrum of HR640 in response to 2H2O suspension indicates that the Schiff base linkage to the protein is protonated. None of the HR640 fingerprint vibrations shift significantly in 2H2O, suggesting that the Schiff base adopts a C = N anti configuration; this assignment is supported by the frequency of the C15-2H rocking mode (1002 cm-1). The 13-cis structure for the chromophore in HR640 requires that thermal isomerization back to all-trans occurs in the HR640-->HR578 transition. These structural and kinetic results are incorporated into a two-state C-T model for Cl- pumping.     

Effects of various anions on the Raman spectrum of halorhodopsin.

Resonance Raman experiments were conducted to probe and understand the effect of various anions on halorhodopsin. These included monoatomic anions Cl- and Br-, which bind to the so-called halorhodopsin binding sites I and II, and polyatomic anions NO3- and ClO4-, which bind to site I only. The two types of ions clearly show different effects on the vibrational spectrum of the chromophore. The differences are not localized to the Schiff base region of the molecule, but extend to the chromophore structure-sensitive fingerprint region as well. We find that the protonated Schiff base frequency is at 1,633 cm-1 for Cl- and Br- ions, as reported previously for Cl-. However, we find that two Schiff base frequencies characterize halorhodopsin upon binding of the polyatomic anions. One frequency lies at the same location as that found for the monoatomic anions and the other is at 1,645 cm-1. Halorhodopsin with bound NO3- and ClO4- thus may consist of two heterogeneous structures in equilibrium. This heterogeneity does not seem to correlate with a retinal isomeric heterogeneity, which we can also demonstrate in these samples. The results suggest that anions binding to site I do not bind to the Schiff base directly, but can influence chromophore and/or protein conformational states.     

Structure and protein environment of the retinal chromophore in light- and dark-adapted bacteriorhodopsin studied by solid-state NMR

Our previous solid-state 13C NMR studies on bR have been directed at characterizing the structure and protein environment of the retinal chromophore in bR568 and bR548, the two components of the dark-adapted protein. In this paper, we extend these studies by presenting solid-state NMR spectra of light-adapted bR (bR568) and examining in more detail the chemical shift anisotropy of the retinal resonances near the ionone ring and Schiff base. Magic angle spinning (MAS) 13C NMR spectra were obtained of bR568, regenerated with retinal specifically 13C labeled at positions 12-15, which allowed assignment of the resonances observed in the dark-adapted bR spectrum. Of particular interest are the assignments of the 13C-13 and 13C-15 resonances. The 13C-15 chemical resonance for bR568 (160.0 ppm) is upfield of the 13C-15 resonance for bR548 (163.3 ppm). This difference is attributed to a weaker interaction between the Schiff base and its associated counterion in bR568. The 13C-13 chemical shift for bR568 (164.8 ppm) is close to that of the all-trans-retinal protonated Schiff base (PSB) model compound (approximately 162 ppm), while the 13C-13 resonance for bR548 (168.7 ppm) is approximately 7 ppm downfield of that of the 13-cis PSB model compound. The difference in the 13C-13 chemical shift between bR568 and bR548 is opposite that expected from the corresponding 15N chemical shifts of the Schiff base nitrogen and may be due to conformational distortion of the chromophore in the C13 = C14-C15 bonds.(ABSTRACT TRUNCATED AT 250 WORDS)     

Resonance raman spectroscopy of an ultraviolet-sensitive insect rhodopsin

We present the first visual pigment resonance Raman spectra from the UV-sensitive eyes of an insect, Ascalaphus macaronius (owlfly). This pigment contains 11-cis-retinal as the chromophore. Raman data have been obtained for the acid metarhodopsin at 10 degrees C in both H2O and D2O. The C = N stretching mode at 1660 cm-1 in H2O shifts to 1631 cm-1 upon deuteriation of the sample, clearly showing a protonated Schiff base linkage between the chromophore and the protein. The structure-sensitive fingerprint region shows similarities to the all-trans-protonated Schiff base of model retinal chromophores, as well as to the octopus acid metarhodopsin and bovine metarhodopsin I. Although spectra measured at -100 degrees C with 406.7-nm excitation, to enhance scattering from rhodopsin (lambda max 345 nm), contain a significant contribution from a small amount of contaminants [cytochrome(s) and/or accessory pigment] in the sample, the C = N stretch at 1664 cm-1 suggests a protonated Schiff base linkage between the chromophore and the protein in rhodopsin as well. For comparison, this mode also appears at approximately 1660 cm-1 in both the vertebrate (bovine) and the invertebrate (octopus) rhodopsins. These data are particularly interesting since the absorption maximum of 345 nm for rhodopsin might be expected to originate from an unprotonated Schiff base linkage. That the Schiff base linkage in the owlfly rhodopsin, like in bovine and in octopus, is protonated suggests that a charged chromophore is essential to visual transduction.     

Effect of lipid-protein interaction on the color of bacteriorhodopsin

Detergent solubilization and subsequent delipidation of bacteriorhodopsin (bR) results in the formation of a new species absorbing maximally at 480 nm (bR480). Upon lowering the pH, its absorption shifts to 540 nm (bR540). The pK of this equilibrium is 2.6, with the higher pH favoring bR480 (Baribeau, J. and Boucher, F. (1987) Biochim. Biophysica Acta, 890, 275-278). Resonance Raman spectroscopy shows that bR480, like the native bR, contains a protonated Schiff base (PSB) linkage between the chromophore and the protein. However, the Schiff base vibrational frequency in bR480, and its shift upon deuteration, are quite different from these in the native bR, suggesting changes in the Schiff base environment upon delipidation. Infrared absorption and circular-dichroism (CD) spectral studies do not show any net change in the protein secondary structure upon formation of bR480. It is shown that deprotonation of the Schiff base is not the only mechanism of producing hypsochromic shift in the absorption maximum of bR-derived pigments, subtle changes in the protein tertiary structure, affecting the Schiff base environment of the chromophore, may play an equally significant role in the color regulation of bR-derived pigments.     

Hydrogen-bonding alterations of the protonated Schiff base and water molecule in the chloride pump of Natronobacterium pharaonis

Halorhodopsin is a light-driven chloride ion pump. Chloride ion is bound in the Schiff base region of the retinal chromophore, and unidirectional chloride transport is probably enforced by the specific hydrogen-bonding interaction with the protonated Schiff base and internal water molecules. In this article, we study hydrogen-bonding alterations of the Schiff base and water molecules in halorhodopsin of Natronobacterium pharaonis (pHR) by assigning their N-D and O-D stretching vibrations in D(2)O, respectively. Highly accurate low-temperature Fourier transform infrared spectroscopy revealed that hydrogen bonds of the Schiff base and water molecules are weak in the unphotolyzed state, whereas they are strengthened upon retinal photoisomerization. Halide dependence of the stretching vibrations enabled us to conclude that the Schiff base forms a direct hydrogen bond with Cl(-) only in the K intermediate. Hydrogen bond of the Schiff base is further strengthened in the L(1) intermediate, whereas the halide dependence revealed that the acceptor is not Cl(-), but presumably a water molecule. Thus, it is concluded that the hydrogen-bonding interaction between the Schiff base and Cl(-) is not a driving force of the motion of Cl(-). Rather, the removal of its hydrogen bonds with the Schiff base and water(s) makes the environment around Cl(-) less polar in the L(1) intermediate, which presumably drives the motion of Cl(-) from its binding site to the cytoplasmic domain.     

Vibrational analysis of the all-trans retinal protonated Schiff base.

We have obtained Raman spectra of a series of all-trans retinal protonated Schiff-base isotopic derivatives. 13C-substitutions were made at the 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, and 15 positions while deuteration was performed at position 15. Based on the isotopic shifts, the observed C--C stretching vibrations in the 1,100-1,400 cm-1 fingerprint region are assigned. Normal mode calculations using a modified Urey-Bradley force field have been refined to reproduce the observed frequencies and isotopic shifts. Comparison with fingerprint assignments of all-trans retinal and its unprotonated Schiff base shows that the major effect of Schiff-base formation is a shift of the C14--C15 stretch from 1,111 cm-1 in the aldehyde to approximately 1,163 cm-1 in the Shiff base. This shift is attributed to the increased C14--C15 bond order that results from the reduced electronegativity of the Schiff-base nitrogen compared with the aldehyde oxygen. Protonation of the Schiff base increases pi-electron delocalization, causing a 6 to 16 cm-1 frequency increase of the normal modes involving the C8--C9, C10--C11, C12--C13, and C14--C15 stretches. Comparison of the protonated Schiff base Raman spectrum with that of light-adapted bacteriorhodopsin (BR568) shows that incorporation of the all-trans protonated Schiff base into bacterio-opsin produces an additional approximately 10 cm-1 increase of each C--C stretching frequency as a result of protein-induced pi-electron delocalization. Importantly, the frequency ordering and spacing of the C--C stretches in BR568 is the same as that found in the protonated Schiff base.     

Chromophore structure in bacteriorhodopsin's N intermediate: implications for the proton-pumping mechanism

By elevating the pH to 9.5 in 3 M KCl, the concentration of the N intermediate in the bacteriorhodopsin photocycle has been enhanced, and time-resolved resonance Raman spectra of this intermediate have been obtained. Kinetic Raman measurements show that N appears with a half-time of 4 +/- 2 ms, which agrees satisfactorily with our measured decay time of the M412 intermediate (2 +/- 1 ms). This argues that M412 decays directly to N in the light-adapted photocycle. The configuration of the chromophore about the C13 = C14 bond was examined by regenerating the protein with [12,14-2H]retinal. The coupled C12-2H + C14-2H rock at 946 cm-1 demonstrates that the chromophore in N is 13-cis. The shift of the 1642-cm-1 Schiff base stretching mode to 1618 cm-1 in D2O indicates that the Schiff base linkage to the protein is protonated. The insensitivity of the 1168-cm-1 C14-C15 stretching mode to N-deuteriation establishes a C = N anti (trans) Schiff base configuration. The high frequency of the C14-C15 stretching mode as well as the frequency of the 966-cm-1 C14-2H-C15-2H rocking mode shows that the chromophore is 14-s-trans. Thus, N contains a 13-cis, 14-s-trans, 15-anti protonated retinal Schiff base.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fourier transform infrared evidence for Schiff base alteration in the first step of the bacteriorhodopsin photocycle

The first step of the bacteriorhodopsin (bR) photocycle involves the formation of a red-shifted product, K. Fourier transform infrared difference spectra of the bR570 to K630 transition at 81 K has been measured for bR containing different isotopic substitutions at the retinal Schiff base. In the case of bacteriorhodopsin containing a deuterium substitution at the Schiff base nitrogen, carbon 15, or both, we find spectral changes in the 1600-1610- and 1570-1580-cm-1 region consistent with the hypothesis that the K630 C=N stretching mode of a protonated Schiff base is located near 1609 cm-1. A similar set of Schiff base deuterium substitutions for retinal containing a 13C at the carbon 10 position strongly supports this conclusion. This assignment of the K630 C=N stretching vibration provides evidence that the bR Schiff base proton undergoes a substantial environmental change most likely due to separation from a counterion. In addition, a correlation is found between the C=N stretching frequency and the maximum wavelength of visible absorption, suggesting that movement of a counterion relative to the Schiff base proton is the main source of absorption changes in the early stages of the photocycle. Such a movement is a key prediction of several models of proton transport and energy transduction. Evidence is also presented that one or more COOH groups are involved in the formation of the K intermediate.     

Fourier transform infrared study of the halorhodopsin chloride pump

Halorhodopsin (hR) is a light-driven chloride pump located in the cell membrane of Halobacterium halobium. Fourier transform infrared difference spectroscopy has been used to study structural alterations occurring during the hR photocycle. The frequencies of peaks attributed to the retinylidene chromophore are similar to those observed in the spectra of the related protein bacteriorhodopsin (bR), indicating that in hR as in bR an all-trans----13-cis isomerization occurs during formation of the early bathoproduct. Spectral features due to protein structural alterations are also similar for the bR and hR photocycles. For example, formation of the red-shifted primary photoproducts of both hR and bR results in similar carboxyl peaks in the 1730-1745-cm-1 region. However, in contrast to bR, no further changes are observed in the carboxyl region during subsequent steps in the hR photocycle, indicating that additional carboxyl groups are not directly involved in chloride translocation. Overall, the close similarity of vibrations in hR and bR photoproduct difference spectra supports the existence of some common elements in the molecular mechanisms of energy transduction and active transport by these two proteins.     

Factors affecting the C = N stretching in protonated retinal Schiff base: a model study for bacteriorhodopsin and visual pigments

Factors affecting the C = N stretching frequency of protonated retinal Schiff base (RSBH+) were studied with a series of synthetic chromophores and measured under different conditions. Interaction of RSBH+ with nonconjugated positive charges in the vicinity of the ring moiety or a planar polyene conformation (in contrast to the twisted retinal conformation in solution) shifted the absorption maxima but did not affect the C = N stretching frequency. The latter, however, was affected by environmental perturbations in the vicinity of the Schiff base linkage. Diminished ion pairing (i.e., of the positively charged nitrogen to its anion) achieved either by substituting a more bulky counteranion or by designing models with a homoconjugation effect lowered the C = N stretch energy. Decreasing solvation of the positively charged nitrogen leads to a similar trend. These effects in the vicinity of the Schiff base linkage also perturb the deuterium isotope effect observed upon deuteriation of the Schiff base. The results are interpreted by considering the mixing of the C = N stretching and C = N-H bending vibration. The C = N mode is shifted due to electrostatic interaction with nonconjugated positive charges in the vicinity of the Schiff base linkage, an interaction that does not influence the isotope effect. Weak hydrogen bonding between the Schiff base linkage in bacteriorhodopsin (bR) and its counteranion or, alternatively, poor solvation of the positively charged Schiff base nitrogen can account for the C = N stretching frequency of 1640 cm-1 and the deuterium isotope effect of 17 cm-1 observed in this pigment.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structure of the retinal chromophore in 7,9-dicis-rhodopsin

Bovine rhodopsin was bleached and regenerated with 7,9-dicis-retinal to form 7,9-dicis-rhodopsin, which was purified on a concanavalin A affinity column. The absorption maximum of the 7,9-dicis pigment is 453 nm, giving an opsin shift of 1600 cm-1 compared to 2500 cm-1 for 11-cis-rhodopsin and 2400 cm-1 for 9-cis-rhodopsin. Rapid-flow resonance Raman spectra have been obtained of 7,9-dicis-rhodopsin in H2O and D2O at room temperature. The shift of the 1654-cm-1 C = N stretch to 1627 cm-1 in D2O demonstrates that the Schiff base nitrogen is protonated. The absence of any shift in the 1201-cm-1 mode, which is assigned as the C14-C15 stretch, or of any other C-C stretching modes in D2O indicates that the Schiff base C = N configuration is trans (anti). Assuming that the cyclohexenyl ring binds with the same orientation in 7,9-dicis-, 9-cis-, and 11-cis-rhodopsins, the presence of two cis bonds requires that the N-H bond of the 7,9-dicis chromophore points in the opposite direction from that in the 9-cis or 11-cis pigment. However, the Schiff base C = NH+ stretching frequency and its D2O shift in 7,9-dicis-rhodopsin are very similar to those in 11-cis- and 9-cis-rhodopsin, indicating that the Schiff base electrostatic/hydrogen-bonding environments are effectively the same. The C = N trans (anti) Schiff base geometry of 7,9-dicis-rhodopsin and the insensitivity of its Schiff base vibrational properties to orientation are rationalized by examining the binding site specificity with molecular modeling.     

Resonance Raman study of the pink membrane photochemically prepared from the deionized blue membrane of H. halobium.

We report here the Resonance Raman spectrum of a 'pink' membrane (lambda max approximately 495 nm) photochemically generated from the deionized 'blue' membrane (Chang et al., 1985). Comparison of the Raman spectrum of the pink membrane with that of the model compounds, as well as the chromophore extraction data, indicate that the chromophore in the pink membrane is in the 9-cis configuration. The Schiff base peak at approximately 1,652 cm-1 shifts to approximately 1,622 cm-1 upon deuteration of the pink membrane, showing that the chromophore is bound to the bacterio-opsin by a protonated Schiff base linkage. The location of the Schiff base peak, as well as the 30 cm-1 shift that it undergoes upon deuteration, are quite different from the corresponding values for the native bacteriorhodopsin, suggesting differences in the local environment for the Schiff base in these pigments.     

Determination of retinal chromophore structure in bacteriorhodopsin with resonance Raman spectroscopy

The analysis of the vibrational spectrum of the retinal chromophore in bacteriorhodopsin with isotopic derivatives provides a powerful "structural dictionary" for the translation of vibrational frequencies and intensities into structural information. Of importance for the proton-pumping mechanism is the unambiguous determination of the configuration about the C13=C14 and C=N bonds, and the protonation state of the Schiff base nitrogen. Vibrational studies have shown that in light-adapted BR568 the Schiff base nitrogen is protonated and both the C13=C14 and C=N bonds are in a trans geometry. The formation of K625 involves the photochemical isomerization about only the C13=C14 bond which displaces the Schiff base proton into a different protein environment. Subsequent Schiff base deprotonation produces the M412 intermediate. Thermal reisomerization of the C13=C14 bond and reprotonation of the Schiff base occur in the M412------O640 transition, resetting the proton-pumping mechanism. The vibrational spectra can also be used to examine the conformation about the C--C single bonds. The frequency of the C14--C15 stretching vibration in BR568, K625, L550 and O640 argues that the C14--C15 conformation in these intermediates is s-trans. Conformational distortions of the chromophore have been identified in K625 and O640 through the observation of intense hydrogen out-of-plane wagging vibrations in the Raman spectra (see Fig. 2). These two intermediates are the direct products of chromophore isomerization. Thus it appears that following isomerization in a tight protein binding pocket, the chromophore cannot easily relax to a planar geometry. The analogous observation of intense hydrogen out-of-plane modes in the primary photoproduct in vision (Eyring et al., 1982) suggests that this may be a general phenomenon in protein-bound isomerizations. Future resonance Raman studies should provide even more details on how bacterio-opsin and retinal act in concert to produce an efficient light-energy convertor. Important unresolved questions involve the mechanism by which the protein catalyzes deprotonation of the L550 intermediate and the mechanism of the thermal conversion of M412 back to BR568. Also, it has been shown that under conditions of high ionic strength and/or low light intensity two protons are pumped per photocycle (Kuschmitz & Hess, 1981). How might this be accomplished?(ABSTRACT TRUNCATED AT 400 WORDS)     

Vibrational spectroscopy of bacteriorhodopsin mutants: I. Tyrosine-185 protonates and deprotonates during the photocycle

The techniques of FTIR difference spectroscopy and site-directed mutagenesis have been combined to investigate the role of individual tyrosine side chains in the proton-pumping mechanism of bacteriorhodopsin (bR). For each of the 11 possible bR mutants containing a single Tyr----Phe substitution, difference spectra have been obtained for the bR----K and bR----M photoreactions. Only the Tyr-185----Phe mutation results in the disappearance of a set of bands that were previously shown to be due to the protonation of a tyrosinate during the bR----K photoreaction [Rothschild et al.: Proceedings of the National Academy of Sciences of the United States of America 83:347, (1986]). The Tyr-185----Phe mutation also eliminates a set of bands in the bR----M difference spectrum associated with deprotonation of a Tyr; most of these bands (e.g., positive 1272-cm-1 peak) are completely unaffected by the other ten Tyr----Phe mutations. Thus, tyrosinate-185 gains a proton during the bR----K reaction and loses it again when M is formed. Our FTIR spectra also provide evidence that Tyr-185 interacts with the protonated Schiff base linkage of the retinal chromophore, since the negative C = NH+ stretch band shifts from 1640 cm-1 in the wild type to 1636 cm-1 in the Tyr-185----Phe mutant. A model that is consistent with these results is that Tyr-185 is normally ionized and serves as a counter-ion to the protonated Schiff base. The primary photoisomerization of the chromophore translocates the Schiff base away from Tyr-185, which raises the pKa of the latter group and results in its protonation.     

不同pH条件下细菌视紫红质的共振拉曼光谱研究

本实验测定了不同pH条件下嗜盐菌紫膜中细菌视紫红质(bR)的共振拉曼光谱.13-顺式视黄醛生色团的特征峰1187cm~(-1)和全反式、13-顺式共有的特征峰1200cm~(-1)带强度之比I_(1187)/I_(1200)在pH1.0-8.9之间约为0.76,而pH高于8.9为0.97.pH3.0-9.0时C=NH~ 振动峰为1640-1642cm~(-1),pH9.4以上为1642-1644cm~(-1),pH9.2附近变化最大,pH3.0以下低于1640cm~(-1).酸性和弱碱性范围时,19-CH_3和20-CH_3的面内变形振动与面外变形振动相互重叠,碱性范围分为双峰.并讨论了对结构及其稳定性的影响.