Transmembrane location of retinal in bacteriorhodopsin by neutron diffraction

The transmembrane location of the chromophore of bacteriorhodopsin was obtained by neutron diffraction on oriented stacks of purple membranes. Two selectively deuterated retinals were synthesized and incorporated in bacteriorhodopsin by using the retinal- mutant JW5: retinal-d11 (D11) contained 11 deuterons in the cyclohexene ring, and retinal-d5 (D5) had 5 deuterons as close as possible to the Schiff base end of the chromophore. The membrane stacks had a lamellar spacing of 53.1 A at 86% relative humidity. Five orders were observed in the lamellar diffraction pattern of the D11, D5, and nondeuterated reference samples. The reflections were phased by D2O-H2O exchange. The absolute values of the structure factors were nonlinear functions of the D2O content, suggesting that the coherently scattering domains consisted of asymmetric membrane stacks. The centers of deuteration were determined from the observed intensity differences between labeled and unlabeled samples by using model calculations and Fourier difference methods. With the origin of the coordinate system defined midway between consecutive intermembrane water layers, the coordinates of the center of deuteration of the D11 and D5 label are 10.5 +/- 1.2 and 3.8 +/- 1.5 A, respectively. Alternatively, the label distance may be measured from the nearest membrane surface as defined by the maximum in the neutron scattering length density at the water/membrane interface. With respect to this point, the D11 and D5 labels are located at a depth of 9.9 +/- 1.2 and 16.6 +/- 1.5 A, respectively. The chromophore is tilted with the Schiff base near the middle of the membrane and the ring closer to the membrane surface. The vector connecting the two label positions in the chromophore makes an angle of 40 +/- 12 degrees with the plane of the membrane. Of the two possible orientations of the plane of the chromophore, which is perpendicular to the membrane plane, only the one in which the N----H bond of the Schiff base points toward the same membrane surface as the vector from the Schiff base to the cyclohexene ring is compatible with the known tilt angle of the polyene chain.     

Orientation of the bacteriorhodopsin chromophore probed by polarized Fourier transform infrared difference spectroscopy

Polarized, low-temperature Fourier transform infrared (FTIR) difference spectroscopy has been used to investigate the structure of bacteriorhodopsin (bR) as it undergoes phototransitions from the light-adapted state, bR570, to the K630 and M412 intermediates. The orientations of specific retinal chromophore and protein groups relative to the membrane plane were calculated from the linear dichroism of the infrared bands, which correspond to the vibrational modes of those groups. The linear dichroism of the chromophore C=C and C-C stretching modes indicates that the long axis of the polyene chain is oriented at 20-25 degrees from the membrane plane at 250 K and that it orients more in-plane when the temperature is reduced to 81 K. The polyene plane is found to be approximately perpendicular to the membrane plane from the linear dichroism calculations of the HOOP (hydrogen out-of-plane) wags. The orientation of the transition dipole moments of chromophore vibrations in the K630 and M412 intermediates has been probed, and the dipole moment direction of the C=O bond of an aspartic acid that is protonated in the bR570----M412 transition has been measured.     

Polarized absorption spectra of green fluorescent protein single crystals: transition dipole moment directions

Polarized absorption spectra of orthorhombic crystals of wild-type green fluorescent protein (GFP) were measured between 350 and 520 nm to obtain information on the directions of the electronic transition dipole moments ((-->)m) of the chromophore relative to the molecular axes. The transition dipole moment orientation is a basic spectroscopic parameter of relevance to biologists when interpreting F?rster-type fluorescence resonance energy transfer data and for comparing absorbance and fluorescence spectra of GFP with quantum chemical calculations. Maximal extinction was obtained throughout the spectrum when the polarization direction of the electric vector of incident light was parallel to the c-axis of the crystal. The transition dipole moments were assumed to be parallel to the plane of the chromophore. With this assumption and the measured dichroic ratios in the crystals, the transition dipole moments associated with the neutral (lambda(max) = 398 nm) and anionic (lambda(max) = 478 nm) forms of the chromophore were found to subtend angles of approximately 26 degrees and 13 degrees (counterclockwise), respectively, with the vector that joins the phenolic and imidazolinone oxygen atoms of the chromophore.     

Orientation of retinal in purple membrane determined by polarized Raman spectroscopy.

The orientation of the retinal molecule in the purple membrane was determined by polarized Raman spectroscopy for stacked purple membranes. The depolarization ratios of C = C stretching vibration mode were measured for three scattering geometries of purple membrane films. From the depolarization ratios we estimated the tilt angle of the transition dipole moment of retinal to the membrane normal and the rotational angle of the molecular plane along the transition dipole moment of retinal. The molecular plane of M intermediate was found to be almost perpendicular to the membrane plane. We confirmed that the tilt angle was 65 +/- 2 degrees for both bR and M intermediates.     

Transient and linear dichroism studies on bacteriorhodopsin: determination of the orientation of the 568 nm all-trans retinal chromophore

The orientation of the 568 nm transition dipole moment of the retinal chromophore of bacteriorhodopsin has been determined in purple membranes from Halobacterium halobium and in reconstituted vesicles. The angle between the 568 nm transition dipole moment and the normal to the plane of the membrane was measured in two different ways.In the first method the angle was obtained from transient dichroism measurements on bacteriorhodopsin incorporated into large phosphatidylcholine vesicles. Following flash excitation with linearly polarized light, the anisotropy of the 568 nm ground-state depletion signal first decays but then reaches a time-independent value. This result, obtained above the lipid phase transition, is interpreted as arising from rotational motion of bacteriorhodopsin which is confined to an axis normal to the plane of the membrane. It is shown that the relative amplitude of the time-independent component depends on the orientation of the 568 nm transition dipole moment. From the data an angle of 78 ° ± 3 ° is determined.In the second method the linear dichroism was measured as a function of the angle of tilt between the oriented purple membranes and the direction of the light beam. The results were corrected for the angular distribution of the membranes within the oriented samples, which was determined from the mosaic spread of the first-order lamellar neutron diffraction peak. In substantial agreement with the results of the transient dichroism method, linear dichroism measurements on oriented samples lead to an angle of 71 ° ± 4 °.No significant wavelength dependence of the dichroic ratio across the 568 nm band was observed, implying that the exciton splitting in this band must be substantially smaller than the recently suggested value of 20 nm (Ebrey et al., 1977).The orientation of the 568 nm transition dipole moment, which coincides with the direction of the all-trans polyene chain of retinal, is not only of interest in connection with models for the proton pump, but can also be used to calculate the inter-chromophore distances in the purple membrane.     

Structure determination of the cyclohexene ring of retinal in bacteriorhodopsin by solid-state deuterium NMR.

The orientation and conformation of retinal within bacteriorhodopsin of the purple membrane of Halobacterium halobium was established by solid-state deuterium NMR spectroscopy, through the determination of individual chemical bond vectors. The chromophore ([2,4,4,16,16,17,17,17,18,18-2H11]retinal) was specifically deuterium-labeled on the cyclohexene ring and incorporated into the protein. A uniaxially oriented sample of purple membrane patches was prepared and measured at a series of inclinations relative to the spectrometer field. 31P NMR was used to characterize the mosaic spread of the oriented sample, and computer simulations were applied in the analysis of the 2H NMR and 31P NMR spectral line shapes. From the deuterium quadrupole splittings, the specific orientations of the three labeled methyl groups on the cyclohexene ring could be calculated. The two adjacent methyl groups (on C1) of the retinal were found to lie approximately horizontal in the membrane and make respective angles of 94 degrees +/- 2 degrees and 75 degrees +/- 2 degrees with the membrane normal. The third group (on C5) points toward the cytoplasmic side with an angle of 46 degrees +/- 3 degrees. These intramolecular constraints indicate that the cyclohexene ring lies approximately perpendicular to the membrane surface and that it has a (6S)-trans conformation. From the estimated angle of the tilt of the chomophore long axis, it is concluded that the polyene chain is slightly curved downward to the extracellular side of the membrane.     

Infrared dichroism from the X-ray structure of bacteriorhodopsin

A detailed comparison with the three-dimensional protein structure provides a stringent test of the models and parameters commonly used in determining the orientation of the alpha-helices from the linear dichroism of the infrared amide bands, particularly in membranes. The order parameters of the amide vibrational transition moments are calculated for the transmembrane alpha-helices of bacteriorhodopsin by using the crystal structure determined at a resolution of 1.55 A (PDB accession number 1C3W). The dependence on the angle delta(M) that the transition moment makes with the peptide carbonyl bond is fit by the expression ((3)/(2)S(alpha) cos(2) alpha)cos(2)(delta(M) + beta) - 1/2S(alpha), where S(alpha) (0.91) is the order parameter of the alpha-helices, alpha (13 degrees ) is the angle that the peptide plane makes with the helix axis, and beta (11 degrees ) is the angle that the peptide carbonyl bond makes with the projection of the helix axis on the peptide plane. This result is fully consistent with the model of nested axial distributions commonly used in interpreting infrared linear dichroism of proteins. Comparison with experimental infrared dichroic ratios for bacteriorhodopsin yields values of Theta(A) = 33 +/- 1 degree, Theta(I) = 39.5 +/- 1 degree, and Theta(II) = 70 +/- 2 degrees for the orientation of the transition moments of the amide A, amide I, and amide II bands, respectively, relative to the helix axis. These estimates are close to those found for model alpha-helical polypeptides, indicating that side-chain heterogeneity and slight helix imperfections are unlikely to affect the reliability of infrared measurements of helix orientations.     

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.     

Linear dichroism of rhodopsin in air-water interface films

Air-water interface films of purified cattle rhodopsin and defined phospholipids are formed by the osmotic lysis of reconstituted membrane vesicles. The interface films thus formed consist of a phospholipid monolayer containing vesicle membrane fragments. Rhodopsin molecules at the interface are restricted within the membrane fragments where they are spectrophotometrically intact and capable of undergoing photoregeneration and chemical regeneration. Multilayers of up to 8 layers can be built from these interface films. The visible absorption band of rhodopsin in these multilayers is linearly dichroic. Quantitative analysis of the linear dichroism reveals that the dipole moment of transition of the retinal chromophore in rhodopsin forms an angle of 15 degrees +/- 4 degrees with the plane of the membrane fragments in the interface film. This orientation of the chromophore relative to the plane of the membrane is essentially the same as that observed in the intact retina. Thus, the orientation of rhodopsin in the interface films is similar to that in the intact disc membranes.     

Vibrational frequency and dipolar orientation of the protonated Schiff base in bacteriorhodopsin before and after photoisomerization

Light-driven proton transport in bacteriorhodopsin (BR) is initiated by photoisomerization of the retinylidene chromophore, which perturbs the hydrogen bonding network in the Schiff base region of the active site. This study aimed to identify the frequency and dipolar orientation of the N-D stretching vibrations of the Schiff base before and after photoisomerization, by means of low-temperature polarized FTIR spectroscopy of [zeta-(15)N]lysine-labeled BR in D(2)O. (15)N-shifted modes were found at 2123 and 2173 cm(-1) for BR, and at 2468 and 2495 cm(-1) for the K intermediate. The corresponding N-H stretches are at approximately 2800 cm(-1) for BR and 3350-3310 cm(-1) for the K intermediate. The shift to a 350 cm(-1) higher frequency upon photoisomerization is consistent with loss of the hydrogen bond of the Schiff base. The N-D stretch frequencies of the Schiff base in BR and the K intermediate are close to the O-D stretch frequencies of strongly hydrogen bonded water and Thr89, respectively. The angles of the dipole moments of the N-D stretches to the membrane normal were determined to be 60-65 degrees for BR and approximately 90 degrees for the K intermediate. In the case of BR, the stretch orientation is expected to deviate from the N-D bond orientation due to vibrational mixing in the hydrogen bonding network. In contrast, the data for the K intermediate suggest that the N-D group is not hydrogen bonded and orients along the membrane.     

Orientation of carotenoids in the outer membrane of Synechocystis PCC 6714 (cyanobacteria)

The orientation of outer membrane carotenoids from Synechocystis PCC 6714 and Synechococcus PCC 6307 was studied by linear dichroism spectrophotometry. Uniaxially oriented, tilted outer membrane films revealed a significant linear dichroism after rotating the polarization vector of the incident light beam, indicating a predominant orientation of the carotenoid transition moments perpendicular to the outer membrane plane. Values for the reduced dichroism at the absorbance maxima presented a linear correlation to a function of the tilt angle (sin2 alpha).     

Interpretation of the absorption and circular dichroic spectra of oriented purple membrane films.

The absorption and circular dichroic (CD) spectra of purple membrane films in which the plane of the membranes is oriented perpendicular to the incident beam are compared with the solution spectra. This enables one to relate structural features of the purple membrane to a coordinate system as defined by a normal to the membrane plane and two mutually perpendicular in-plane axes. The film and solution absorption spectra were similar except for a relative depression in the 200 - 225-nm region of the film spectrum. However, the CD spectra showed significant differences in the visible region, where the biphasic band in the solution spectrum was replaced by a single positive band at 555 nm in the film spectrum and in the far ultraviolet region, where the 208-nm band was deleted from the film spectra of the native and regenerated membranes. Moreover, a small shoulder occurred at 208 nm in the film spectrum of the bleached membrane. The near ultraviolet spectra also showed differences, whereas the 317-nm band remained essentially the same for both spectra. Based on excitonic interpretations of the visible and far ultraviolet spectra the following conclusions were reached: (a) a relatively strong in-plane monomeric interaction occurs between te retinyl chromophore and apoprotein; (b) the helical axes of the native and regenerated membrane proteins are oriented primarily normal to the membrane plane; and (c) the helical axes of the bleached membrane proteins are tilted more in-plane than the axes of the native or regenerated membrane. Additional conclusions were that an interaction occurs between an in-plane magnetic dipole moment of the retinyl chromophore and probably an in-plane electric dipole moment of a nearby aromatic amino acid(s), and that although the membrane is anisotropic with respect to coupling between electric and magnetic moments of the aromatic amino acids, the transition dipole moments of the aromatic amino acids are not preferentially oriented in either direction.     

The orientations of reaction center transition moments in the chromatophore membrane of Rhodopseudomonas sphareroides, bases on new linear dichroism and photoselection measurements.

Chromatophore membranes from Rhodopseudomonas sphaeroides were oriented by drying suspensions on the surfaces of glass slides, Polarized spectra of light-induced absorption changes were obtained between 500 and 1000 nm. As observed earlier, these spectra showed negative bands, reflecting photooxidation of the bacteriochlorophyll 'special pair' in the reaction centers, centered near 870, 810, 630 and 600 nm. These bands have been designated BY1, BY2, BX1 and BX2, respectively, corresponding to two QY transitions and two QX transitions of the dimeric special pair. We found the BY1 and BX1 transition moments to be parallel (within 20 degrees) to the plane of the membrane, whereas the BX2 moment makes an angle of 55--63 degrees with the plane. Using the photoselection technique we found that the angle between the BY1 and BX1 transition moments is 30 degrees, while that between BY1 and BX2 is 75 degrees. The BX1 and BX2 moments were found to be orthogonal, consistent with the prediction of molecular exciton theory for a dimer. By combining these data, we have calculated the orientations of the transition moments of the bacteriochlorophyll dimer in spherical polar coordinates, with the pole of the coordinate system normal to the plane of the membrane. The orientations of the QY and QX transition moments of the two bacteriopheophytin molecules in the reaction center were also computed in this coordinate system by transforming the data reported by Clayton, C.N., Rafferty, R.K. and Vermeglio, A. ((1979) Biochim. Biophys. Acta 545, 58--68). We have derived the transformation equations for two polar coordinate systems: in one, the pole is an axis of symmetry as defined by the orientations of purified reaction centers in stretched gelatin films (Rafferty, C.N. and Clayton, R.K. (1979) Biochim. Biophys. Acta 545, 106--121). In the other, the pole is normal to the plane of the chromatophore membrane. These two polar axes are approximately orthogonal.     

NMR structural analysis of a membrane protein: bacteriorhodopsin peptide backbone orientation and motion

In reconstituted vesicles above the lipid phase transition temperature, bacteriorhodopsin (BR) undergoes rotational diffusion about an axis perpendicular to the plane of the bilayer [Cherry, R. J., Muller, U., & Schneider, G. (1977) FEBS Lett. 80, 465]. This diffusion narrows the 13C NMR powder line shape of the BR peptide carbonyls. In contrast, BR in native purple membrane is relatively immobile and exhibits a rigid-lattice powder line shape. By use of the principal values of the rigid-lattice chemical shift tensor and the motionally narrowed line shape from the reconstituted system, the range of Euler angles of the leucine peptide groups relative to the diffusion axis has been calculated. The experimentally observed line shape is inconsistent with those expected for structures which consist entirely of either alpha helix or beta sheet perpendicular to the membrane or beta sheet tilted at angles up to about 60 degrees from the membrane normal. However, for two more complex structural models, the predicted line shapes agree well with the experimental one. These are, first, a structure consisting entirely of alpha1 helices tilted at 20 degrees from the membrane normal and, second, a combination of 60% alpha II helix perpendicular to the membrane plane and 40% antiparallel beta sheet tilted at 10-20 degrees from the membrane normal. The results also indicate that the peptide backbone of bacteriorhodopsin in native purple membrane is extremely rigid even at 40 degrees. The experiments presented here demonstrate a new approach, using solid-state nuclear magnetic resonance (NMR) methods, for structural studies of transmembrane proteins in fluid membrane environments, either natural or reconstituted.(ABSTRACT TRUNCATED AT 250 WORDS)     

Steady-state fluorescence polarization in planar lipid membranes. Experimental and theoretical analysis of the fluorophores 8-anilino-1-naphthalenesulfonate, 1,6-Diphenyl-1,3,5-hexatriene, dansyllysine-valinomycin and n-(9-anthroyloxy) fatty acids

In continuation of earlier work, the steady-state fluorescence polarization in a globally oriented system of planar lipid membranes was analyzed experimentally and theoretically for the fluorophores 8-anilino-1-naphthalenesulfonate, 1,6-diphenyl-1,3, 5-hexatriene, dansyllysine-valinomycin and n-(9-anthroyloxy) fatty acids. The theoretical analyses of experiments were mainly done in terms of the mean orientation of transition moments with respect to the membrane normal, an angle describing the region of hindered rotational diffusion and the coefficients of rotational diffusion perpendicular to the membrane and around the membrane normal. The nonvanishing angle between the moments of absorption and emission was taken into account. In the case of n-(9-anthroyloxy) fatty acids it was found that the orientational disorder increases significantly with the depth of the fluorophore within the membrane. In order to compare with recent results from time-dependent fluorescent polarization in globally isotropic membrane suspensions and with 2H-NMR experiments, the second moment ('order parameter') of the steady-state orientational distribution of absorption dipoles was calculated. For all fluorophores the theoretical analysis indicates a preferred orientation of absorption moments within the membrane plane.     

Polarized fluorescence and absorption of macroscopically aligned Light Harvesting Complex II.

Polarized absorption and fluorescence measurements have been performed at 77 K on isotropic and anisotropic preparations of trimeric Light Harvesting Complex II (LHC-II) from spinach. The results enable a decomposition of the absorption spectrum into components parallel and perpendicular to the trimeric plane. For the first time, it is shown quantitatively that the strong absorption band around 676 nm is polarized essentially parallel to the plane of the trimer, i.e., the average angle between the corresponding transition dipole moments and this plane is at most 12 degrees. The different absorption bands for LHC-II should not be considered as corresponding to individual pigments but to collective excitations of different pigments. Nevertheless, the average angle between the Qy transition dipole moments of all chlorophyll a pigments in LHC-II and the trimeric plane could be determined and was found to be 17.5 degrees +/- 2.5 degrees. For the chlorophyll b pigments, this angle is significantly larger (close to 35 degrees). At 77 K, most of the fluorescence stems from a weak band above 676 nm and the corresponding transition dipole moments are oriented further out of plane than the dipole moments corresponding to the 676-nm band. The results are shown to be of crucial significance for understanding the relation between the LHC-II structure and its spectroscopy.     

The orientation of beta-sheets in porin. A polarized Fourier transform infrared spectroscopic investigation.

The orientation of the protein secondary structures in porin is investigated by Fourier transform infrared (FTIR) linear dichroism of oriented multilayers of porin reconstituted in lipid vesicles. The FTIR absorbance spectrum shows the amide I band at 1,631 cm-1 and several shoulders around 1,675 cm-1 and at 1,696 cm-1 indicative of antiparallel beta-sheets. The amide II is centered around 1,530 cm-1. The main dichroic signals peak at 1,738, 1,698, 1,660, 1,634, and 1,531 cm-1. The small magnitude of the 1,634 cm-1 and 1,531 cm-1 positive dichroism bands demonstrates that the transition moments of the amide I and amide II vibrations are on the average tilted at 47 degrees +/- 3 degrees from the membrane normal. This indicates that the plane of the beta-sheets is approximately perpendicular to the bilayer. From these IR dichroism results and previously reported diffuse x-ray data which revealed that a substantial number of beta-strands are nearly perpendicular to the membrane, a model for the packing of beta-strands in porin is proposed which satisfies both IR and x-ray requirements. In this model, the porin monomer consists of at least two beta-sheet domains, both with their plane perpendicular to the membrane. One sheet has its strands direction lying nearly parallel to the membrane normal while the other sheet has its strands inclined at a small angle away from the membrane plane.     

Linear dichroism of pigments associated with spherical chromatophores. Models of orientation in polyacrylamide gels

Linear dichroism and orientation of pigments in chromatophores of photosynthetic bacteria Chromatium minutissimum and Rhodospirillum rubrum using a novel method of orientation in polyacrylamide gel was studied. A model is proposed for orientation of spherical membranes of chromatophores or other similar vesicules. The value of linear dichroism is derived for known deformation of the gel and a certain angle between the transition dipole and a unit vector perpendicular to the membrane plane. The analysis of linear dichroism spectra permits calculation of angles between the normal to the membrane and the transition dipoles in Chr. minutissimum 65 degrees +/- 1.5 degrees (890 nm absorption band), 63 degrees +/- 1 degree (860 nm), 63 degrees +/- 1 degree (800 nm), 45.5 degrees +/- 1 degree (590 nm), 50.5 degrees +/- 0.5 degree (450--550 nm) and in Rsp. rubrum: 71 degrees +/- 1.5 degree (890 nm), 66.5 degrees +/- 1 degree (870 nm), 69 degrees +/- 1.5 degree (800 nm), 37 degrees +/- 0.5 degree (590 nm), 49.5 degrees +/- 0.5 degree (450--550 nm). The 860 nm band shift to shorter wave-lengths observed in Chr. minutissimum chromatophores treated with 0.01 M potassium ferricyanide is not related to reorientation of transition dipoles, but rather to certain changes of lipid-protein environment.     

Orientation of the tyrosyl D, pheophytin anion, and semiquinone Q(A)(*)(-) radicals in photosystem II determined by high-field electron paramagnetic resonance

The radical forms of two cofactors and an amino acid in the photosystem II (PS II) reaction center were studied by using high-field EPR both in frozen solution and in oriented multilayers. Their orientation with respect to the membrane was determined by using one-dimensionally oriented samples. The ring plane of the stable tyrosyl radical, Y(D)(*), makes an angle of 64 degrees +/- 5 degrees with the membrane plane, and the C-O direction is tilted by 72 degrees +/- 5 degrees in the plane of the radical compared to the membrane plane. The semiquinone, Q(A)(*)(-), generated by chemical reduction in samples lacking the non-heme iron, has its ring plane at an angle of 72 degrees +/- 5 degrees to the membrane plane, and the O-O axis is tilted by 21 degrees +/- 5 degrees in the plane of the quinone compared to the membrane plane. This orientation is similar to that of Q(A)(*)(-) in purple bacteria reaction centers except for the tilt angle which is slightly bigger. The pheophytin anion was generated by photoaccumulation under reducing conditions. Its ring plane is almost perpendicular to the membrane with an angle of 70 degrees +/- 5 degrees with respect to the membrane plane. This is very similar to the orientation of the pheophytin in purple bacteria reaction centers. The position of the g tensor with respect to the molecule is tentatively assigned for the anion radical on the basis of this comparison. In this work, the treatment of orientation data from EPR spectroscopy applied to one-dimensionally oriented multilayers is examined in detail, and improvements over previous approaches are given.     

Electric dichroism in the purple membrane of Halobacterium halobium.

Aqueous suspensions of fragments of the purple membrane of Halobacterium halobium are exposed to short electric field pulses. The relaxation kinetics of the induced dichroism are studied as a function of environmental factors such as temperature, medium viscosity, and treatment of the membranes with glutaraldehyde and dimethylsulfoxide. The data indicate that the alignment of the retinyl chromophore is due to orientation of the whole membrane fragments with their planes parallel to the electric field, as well as to an intramembrane orientation of bacteriorhodopsin molecules (or of a part of such molecules). Wavelength effects on the dichroic ratio show that weak, out of (membrane) plane components contribute to the chromophore spectrum on the red side (lambda greater than 560 nm) of the main (alpha) absorption band as well as the range of the beta band (lambda less than 480 nm). The former effect is attributed to exciton interactions, while the latter is assigned to the contribution of a transition to the lowest 1Ag+ state ("cis" band). It is also concluded that the transition moment along the short (kappa) axis, in the plane of the polyene molecule, has a substantial component perpendicular to the membrane plane.