Resonance Raman spectra of chlorophylls dissolved in liquid crystal matrices. II. Order parameters of chlorophyll a in an MBBA + EBBA liquid crystalline mixture

The molecular ordering of molecules embedded in a uniaxial liquid crystalline system has been considered. In particular, planar Chl a molecules in an MBBA + EBBA mixture have been studied by using polarized resonance Raman spectroscopy. The second- and fourth-rank order parameters and the orientational distribution function of Chl a in the nematic MBBA + EBBA liquid crystalline phase are discussed.     

Resonance Raman spectra of chlorophylls dissolved in liquid crystal matrices. III. Orientational distribution function of chlorophyll b in an MBBA + EBBA liquid crystalline matrix

Polarized resonance Raman spectra of chlorophyll (Chl) b oriented in a mixture of p-methoxybenzylideno-p'-butylaniline (MBBA) and p-ethoxybenzylideno-p'-butylaniline (EBBA) have been measured. The spectra have been analyzed and the second- and fourth-rank order parameters and the orientational distribution function of Chl b are presented.     

Sugar interaction with metal ions. The crystal structure and Raman spectra study of SmCl3-galactitol complex

The crystal structure of 2SmCl3.galactitol.14H2O has been determined. The crystal system is triclinic, space group: P-1. The unit cell dimensions: a = 9.683(2) A, b = 10.341(2) A, c = 7.990(2) A; alpha = 108.01(3) degrees, beta = 92.71(3) degrees, gamma = 88.42(3) degrees. Each Sm atom is coordinated to nine oxygen atoms, three from the alditol and six from water molecules, with Sm-O distance from 2.417 to 2.520 A. The seventh water molecule is hydrogen-bonded by the hydroxy hydrogen on O-3 (O(3)-H(13)...O(10), 2.635 A). After forming complexes the peaks have shifted and the relative intensities have changed in the IR and Raman spectra, which are corresponding to the changes in bond distances and bond angles of the structures. The IR and Raman spectra of Pr-, Nd- and Sm-galactitol complexes are similar, which show that the three metal ions have the same coordination mode.     

Circular dichroism and magnetic circular dichroism spectra of chlorophylls in nematic liquid crystals. I. Electric and weak magnetic field effects on the dichroism spectra

Dichroism spectra of chlorophyll a, chlorophyll b and bacteriochlorophyll a in various nematic liquid crystals are reported. The initial orientation of chlorophylls in such a sample is determined by the interaction of the aggregate formed from the pigment and the liquid crystal molecules with the electrode surface on the cell windows. Reorientation is carried out by either an electric or magnetic field. The analysis of the circular dichroism spectra obtained from these samples on the basis of the Mueller matrix shows that the intensity is predominantly related to the texture of the sample. Chlorophyll molecules can be aggregated with liquid crystals in two ways: (1) through the chlorin magnesium atom, which results in the liquid crystal chain being almost perpendicular to the porphyrin ring, or (2) attached parallel to the line connecting the first and third pyrrole rings of the chlorin, the chlorin now lying in the plane of the liquid crystal chains. By comparing the dichroism spectra of various chlorophylls in the same liquid crystal we can draw conclusions concerning the preferred type of aggregation, not only with liquid crystals, but also with biological molecules. These liquid crystal systems are models of the orientation effects found for chlorophyll in lamellae. The model studied in this work is much simpler than the lamellar system but it does exhibit several common properties with the latter. Both systems are anisotropic and show much more intense dichroism signals, often of opposite sign, compared with those observed for photosynthetic pigments in isotropic solutions. Dichroism signals of organism fragments are much more complex than those of our model, which can either be related to the occurrence in the organism of several types of pigments or, for a given type of pigment, could be the result of exciton splitting. On the basis of our model it is shown that small changes in the anisotropy of the pigment in the surroundings have a strong influence on the sign and amplitude of the observed circular dichroism signal. Such effects may be responsible for the structure of the dichroism spectra observed for biological samples. Such structures can be partially related to the superposition of the dichroism signal from various ‘domains’ of chromophore which are different in both pigment arrangement and in the anisotropy of the surroundings of the pigment molecules themselves.     

Circular dichroism and magnetic circular dichroism spectra of chlorophylls a and b in nematic liquid crystals. II. Magnetic circular dichroism spectra

Absorption and magnetic circular dichroism (MCD) spectra are reported for chlorophyll (Chl) a and Chl b dissolved in nematic liquid crystal solvents. The spectra were measured with the dye molecules oriented uniaxially along the direction of. the magnetic field and measuring light beam. It is significant that under such conditions the MCD spectra recorded in the wavelength region of the Q and Soret bands of the chlorophyll are essentially unchanged with respect to rotation of the sample cell around this axis, even though there is almost complete orientation of the chlorophyll molecules by the liquid crystals. The MCD spectra of Chl a and b in the nematic liquid crystal solvents used in this study are surprisingly similar to the spectra obtained under isotropic conditions. These results illustrate an important technique with which to examine the optical spectra of dyes oriented in liquid crystal matrices in which the anisotropic effects can be reduced the negligible proportions by the application of a strong magnetic field parallel to the direction of the measuring light beam. The first deconvolution calculations are reported that describe the deconvolution of pairs of absorption and MCD spectra, in the Q and B band regions, for both Chl a and b. The spectral analysis to obtain quantitative estimates of transition energies was accomplished by carrying out detailed deconvolution calculations in which the both the absorption and MCD spectral envelopes were fitted with the same number of components; each pair of components had the same hand centres and bandwidth values. This procedure resulted in an assignment of each of the main transitions in the absorption spectra of both Chl a and b. Chl a is clearly monomeric, with Qy, Qx, By and Bx located at 671, 582, 439 and 431 nm, respectively. Analysis of the spectral data for Chl b located Qy, By and Bx, at 662, 476 and 464 nm, respectively.     

Resonance Raman spectra of cytochromes C557 and C558.

Resonance Raman spectra of cytochromes c₅₅₇ and c₅₅₈ have been recorded and compared to other low-spin ferrous cytochromes. The data support the chemical evidence that there is one vinyl group on the heme and one thioether linkage to the protein.     

The stereospecific interaction between chlorophylls and chlorophyllase. Possible implication for chlorophyll biosynthesis and degradation.

Chlorophyllase-catalyzed hydrolysis and esterification of chlorophylls, bacteriochlorophylls, and their free acids, respectively, depend on the configuration around the C-13(2) atom of the corresponding substrate. The data suggest that the enzyme interacts preferentially with compounds having the isocyclic carbomethoxy and the C-17 propionic residues facing opposite sides of the porphyrin macrocycle. The relevance of this observation to chlorophyll biosynthesis and degradation in vivo is briefly discussed.     

Raman spectra and normal vibrations of dipeptides. I. Glycylglycine

We studied the Raman spectra of the zwitterionic glycylglycine crystal (GG) and its N-deuterated analog. A normal coordinate analysis on its α-crystalline form was performed and the effects of intra-and intermolecular couplings are discussed. A modified Urey-Bradley potential was used as a model of the intramolecular force field. Factor group splittings are described by the use of intermolecular potentials consisting of nonbonded atom-atom interactions and dipole-dipole interactions. Effects of hydrogen bonds on the vibrational frequencies of amino and carboxylate groups are also analyzed.     

Resonance Raman spectra of beta-carotene in native and modified low-density lipoprotein

Low-density lipoproteins isolated between density 1.02 and 1.063 g/cm3 from normal fasting human plasma, show strong resonance Raman spectra due to the presence of beta-carotene. Three intense bands, at 1010, 1160 and 1530 cm-1, are assigned to the stretching vibrations of -C-CH3, = C-C = and -C = C- bonds, respectively, of beta-carotene. High-resolution spectra of the 1500-1600 cm-1 region reveal multiple features, suggesting the coexistence of several structural populations of beta-carotene. The modifications of lipoproteins with pH and temperature (30 degrees-42 degrees) change the resonance Raman spectra of beta-carotene. The specific binding of LDL at pH 7.0 by fibroblast cells is suppressed. Our experiments thus suggest that physical and chemical perturbations of plasma lipoproteins modify the lipid-protein interactions and thereby alter the configurational distribution of beta-carotene molecules within these particles.     

Raman spectra of a solid antifreeze glycoprotein and its liquid and frozen aqueous solutions.

Raman spectroscopy was used to study the anomalous decrease in the freezing temperature of water produced by an antifreeze glycoprotein obtained from the sera of an Antarctic fish. An active fraction of this glycoprotein has a molecular weight of approximately 18,000 by equilibrium sedimentation compared to an apparent weight of 20 by freezing temperature depression. The Raman spectra of water present in a 1% antifreeze glycoprotein solution and of ice frozen from this solution were indistinguishable from the spectra of pure water and ice, respectively. These results indicate that the bulk properties of water and ice are unaffected by the presence of the antifreeze glycoprotein. Raman measurements on ice grown slowly, using as seed an oriented single crystal of ice in contact with 1% glycoprotein solutions, showed that the active glycoprotein was not excluded from the ice phase. On the other hand, we found that a smaller, inactive glycoprotein was excluded. Comparison of the Raman spectra of active and inactive glycoprotein components as solids, in 5% solutions, and rapidly frozen 5% solutions, showed that the two components differ in conformation and possibly in the environment of their carbohydrate hydroxyls. These observations suggest that hydrogen bonding of the carbohydrate hydroxyls of the active glycoprotein at the ice-solution interface may physically prevent growth of the ice lattice.     

Resonance Raman spectra of cytochrome c oxidase. Excitation in the 600-nm region.

The resonance Raman (RR) spectra of oxidized, reduced, and oxidized cyanide-bound cytochrome c oxidase with excitation at several wavelengths in the 600-nm region are presented. No evidence is found for laser-induced photoreduction of the oxidized protein with irradiation at lambda approximately 600 nm at 195 K, in contrast to the predominance of this process upon irradiation in the Soret region at this temperature. The Raman spectra of all three protein species are very similar, and there are no Raman bands which are readily assignable to either cytochrome a or cytochrome a3 exclusively. The Raman spectra of the three protein species do, however, exhibit a number of bands not observed in the RR spectra of other hemoproteins upon exicitation in their visible absorption bands. In particular, strong Raman bands are observed in the low-frequency region of the RR spectra (less than 500 cm-1). The frequencies of these bands are similar to those of the copper-ligand vibrations observed in the RR spectra of type 1 copper proteins upon excitation in the 600-nm absorption band characteristic of these proteins. In cytochrome c oxidase, these bands do not disappear upon reduction of the protein and, therefore, cannot be attributed to copper-ligand vibrations. Thus, all the observed RR bands are associated with the two heme A moieties in the enzyme.     

Resonance energy transfer in a model system of membranes: application to gel and liquid crystalline phases.

Resonance energy transfer between octadecyl rhodamine B (donor) and 1,1',3,3,3',3'-hexamethylindotricarbocyanine (acceptor) was studied in a model system of membranes (large unilamellar vesicles of dipalmitoylphosphatidylcholine), using both steady-state and time-resolved techniques. In the fluid phase (temperature = 50 degrees C) the decay law and the steady-state theoretical curve for energy transfer in two dimensions are verified. In the gel phase (temperature = 25 degrees C) an apparent reduction of dimensionality is observed, which is explained on the basis of probe segregation to the defect lines (grain boundaries). An estimation of the domain size from the model recovered linear probe concentrations is approximately 1750-2000 lipid molecules. In both phases, the existence of a fractal geometry was ruled out.     

Time-resolved picosecond fluorescence spectra of the antenna chlorophylls in Chlorella vulgaris. Resolution of Photosystem I fluorescence

The time-resolved fluorescence emission and excitation spectra of Chlorella vulgaris cells have been measured by single-photon timing with picosecond resolution. In a three-exponential analysis the time-resolved excitation spectra recorded at 685 and 706 nm emission wavelength with closed PS II reaction centers show large variations of the preexponential factors of the different decay components as a function of wavelength. At λ_em = 685 nm the major contribution to the fluorescence decay originates from two components with life-times of 2.1–2.4 and 1.2–1.3 ns. A short-lived component with life-times of 0.1–0.16 ns of relatively small amplitude is also found. When the emission is detected at 706 nm, the short-lived component with a life-time of less than 0.1 ns predominates. Time-resolved emission spectra using λ_exc = 630 or λ_exc = 652 nm show a spectral peak of the two longer-lived components at about 680–685 nm, whereas the fast component is red-shifted as compared to the others and shows a maximum at about 690 nm. The emission spectrum observed upon excitation at 696 nm with closed PS II reaction centers shows a large increase in the amplitude of the fast component with a lifetime of 80–100 ps as compared to that at 630 nm excitation. At almost open Photosystem II (PS II) reaction centers (F₀), the life-time of the fast component decreased from 150–160 ps at 682 nm to less than 100 ps at 720 nm emission wavelength. We conclude that at least two pigment pools contribute to the fast component. One is attributed to PS II and the other to Photosystem I (PS I). They have life-times of approx. 180 ps and 80 ps, respectively. The 80 ps (PS I) contribution has a spectral maximum slightly below 700 nm, whereas the 180 ps (PS II) spectrum peaks at 680–685 nm. The spectra of the middle decay component τ_m and its sensitivity to inhibitors of PS II suggest that this component is not preferentially related to LHC II but arises mainly from Chl a pigments probably associated with a second type of PS II centers. The amplitudes of the fast (180 ps, PS II) component and the long-lived decay show an opposite dependence on the state of the PS II centers and confirm our earlier conclusion that the contribution of PS II to the fast component probably disappears at the F_max state (Haehnel W., Holzwarth, A.R. and Wendler, J. (1983) Photochem. Photobiol. 34, 435–443). Our data are discussed in terms of α,β-heterogeneity in PS II centers.     

Raman study of the interaction between polyamines and a GC oligonucleotide.

The interaction between the oligonucleotide d[G(CG)(7)]. d[C(GC)(7)] and the three biogenic polyamines putrescine, spermidine, and spermine under physiological conditions has been studied by Raman spectroscopy. The results indicate the formation of highly ordered aggregated structures in solution, largely stabilized by electrostatic attractions, which have been described as cholesteric phases. Aggregation seems to be preceded by a partial B --> Z conformational transition for spermidine and spermine, which would allow for a deeper oligonucleotide-polyamine interaction. Interaction with the nucleic bases has also been evidenced for aggregates. At low polyamine concentrations the preferential binding sites are similar to those proposed for their interactions with ct-DNA. With increasing the polyamine concentration, the oligonucleotide-polyamine interactions involve both minor and major grooves, which is consistent with the formation of cholesteric phases.