Quantum yield and rate of formation of the carotenoid triplet state in photosynthetic structures

The formation of the triplet state of carotenoids (detected by an absorption peak at 515 nm) and the photo-oxidation of the primary donor of Photosystem II, P-680 (detected by an absorption increase at 820 nm) have been measured by flash absorption spectroscopy in chloroplasts in which the oxygen evolution was inhibited by treatment with Tris. The amount of each transient form has been followed versus excitation flash intensity (at 590 or 694 nm). At low excitation energy the quantum yield of triplet formation (with the Photosystem II reaction center in the state Q⁻) is about 30% that of P-680 photo-oxidation. The yield of carotenoid triplet formation is higher in the state Q⁻ than in the state Q, in nearly the same proportion as chlorophyll a fluorescence. It is concluded that, for excited chlorophyll a, the relative rates of intersystem crossing to the triplet state and of fluorescence emission are the same in vivo as in organic solvent. At high flash intensity the signal of P-680⁺ completely saturates, whereas that of carotenoid triplet continues to increase.

The rate of triplet-triplet energy transfer from chlorophyll a to carotenoids has been derived from the rise time of the absorption change at 515 nm, in chloroplasts and in several light-harvesting pigment-protein complexes. In all cases the rate is very high, around 8 · 10⁷ s⁻¹ at 294 K. It is about 2–3 times slower at 5 K. The transitory formation of chlorophyll triplet has been verified in two pigment-protein complexes, at 5 K.     

Shifts of bacteriochlorophyll and carotenoid absorption bands linked to cytochrome c-555 photooxidation in Chromatium

Shifts in the absorption bands of bacteriochlorophyll and carotenoids in Chromatium vinosum chromatophores were measured after short actinic flashes, under various conditions. The amplitude of the bacteriochlorophyll band shift correlated well with the amount of cytochrome c-555 that was oxidized by P₈₇₀⁺ after a flash. No bacteriochlorophyll band shift appeared to accompany the photooxidation of P₈₇₀ itself, nor the oxidation of cytochrome c-552 by P₈₇₀⁺. The carotenoid band shift also correlated with cytochrome c-555 photooxidation, although a comparatively small carotenoid shift did occur at high redox potentials that permitted only P₈₇₀ oxidation.

The results explain earlier observations on infrared absorbance changes that had suggested the existence of two different photochemical systems in Chromatium. A single photochemical system accounts for all of the absorbance changes.

Previous work has shown that the photooxidations of P₈₇₀ and cytochrome c-555 cause similar changes in the electrical charge on the chromatophore membrane. The specific association of the band shifts with cytochrome c-555 photooxidation therefore argues against interpretations of the band shifts based on a light-induced membrane potential.     

Fusion of proteoliposomes containing the B800-850 light-harvesting complex with membranes of the mutant strain NK3 of Rhodopseudomonas capsulata lacking B800-850

Intracytoplasmic membranes of the mutant strain NK3 of Rhodopseudomonas capsulata lacking the lightharvesting complex B800-850 were fused with proteoliposomes containing the B800-850 complex. Fluorescence emission spectroscopy at 77K showed that after fusion the fluorescence of the B850 bacteriochlorophyll disappeared nearly completely and the B870 fluorescence became prominent. This result and control experiments with proteoliposome-chromatophore mixture and with chromatophore and solubilized B800-850 complexes, respectively, indicate that in fused membranes a reorientation of membrane particles took place and excitons migrated from B850 to B870 bacteriochlorophyll.In fused proteoliposome-chromatophore vesicles a light-induced carotenoid band shift was observed, reflecting the building of an electrical membrane potential due to chargeseparation. Carotenoid band shift was not observed in separated proteoliposomes and NK3 chromatophores.It is concluded that by membrane fusion and lateral diffusion of membrane particles reaction center-light-harvesting B870 complexes came in functional contact with B800-850 antenna complexes.Abbreviations Bchl bacteriochlorophyll - LDAO lauryl dimethylamine oxide - RC reaction center Dedicated to Professor R. Clinton Fuller, Amherst, MA, USA, on the occasion of his 60th birthday in recognition of his work on photosynthetic bacteria and the cooperation between our laboratories     

Blue and red shifts of bacteriochlorophyll absorption band around 880 nm in Rhodospirillum rubrum

The redox potential dependence of the light-induced absorption changes of bacteriochlorophyll in chromatophores and subchromatophore pigment-protein complexes from Rhodospirillum rubrum has been examined. The highest values of the absorption changes due to the bleaching of P-870 and the blue shift of P-800 in chromatophores and subchromatophore complexes are observed in the 360–410 mV redox potential range. At potentials below 300 mV (pH 7.0), the 880 nm band of bacteriochlorophyll shifts to shorter wavelengths in subchromatophore complexes and to longer wavelengths in chromatophores.

The data on redox titration show that the red and blue shifts of 880-nm bacteriochlorophyll band represent the action of a non-identified component (C₃₄₀) which has an oxidation-reduction midpoint potential close to 340 mV (n = 1) at pH 6.0–7.6. The E_m of this component varies by 60 mV/pH unit between pH 7.6 and 9.2.

The results suggest that the red shift is due to the transmembrane, and the blue shift to the local intramembrane electrical field. The generation of both the transmembrane and local electrical fields is apparently governed by redox transitions of the component C₃₄₀.     

Fluorescence emission spectra of cells and subcellular preparations of a green photosynthetic bacterium. Effects of dithionite on the intensity of the emission bands

Fluorescence emission spectra were measured of intact cells and subcellular preparations of the green photosynthetic bacterium Prosthecochloris aestuarii in the presence and in the absence of dithionite. A 3–5-fold increase in bacteriochlorophyll a fluorescence at 816 nm occurred upon addition of dithionite in a membrane vesicle preparation (Complex I), in a photochemically active pigment-protein complex and in a bacteriochlorophyll a protein complex free from reaction centers. The pigment-protein complex showed a relatively strong long-wave emission band (835 nm) of bacteriochlorophyll a, which was preferentially excited by light absorbed at 670 nm and was not stimulated by dithionite. With Complex I, which contains some bacteriochlorophyll c in addition to bacteriochlorophyll a, a 3–4-fold stimulation of bacteriochlorophyll c emission was also observed. Emission bands at shorter wavelengths, probably due to artefacts, were quenched by dithionite. With intact cells, the effect of dithionite was smaller, and consisted mainly of an increase of bacteriochlorophyll a emission.

The results indicate that the strong increase in the yield of bacteriochlorophyll emission that occurred upon generating reducing conditions is, at least mainly, due to a direct effect on the light-harvesting systems, and does not involve the reaction center as had been earlier postulated.     

Fluorescence and energy transfer in phycobiliprotein-containing algae at low temperature

Fluorescence emission spectra of Anacystis nidulans, Porphyridium cruentum and Cyanidium caldarium, three phycobiliprotein-containing algae, were measured at temperatures between 4 and 120 K in the absence and in the presence of quinones as quenchers of chlorophyll fluorescence. In all species three major emission bands were observed in the chlorophyll a region, near 685 nm (F-685), 695 nm (F-695) and between 710 and 730 nm. Additional bands were observed at shorter wavelengths; these were preferentially excited by light absorbed by the phycobiliproteins and are presumably due to phycocyanins and allophycocyanins.

The amplitudes of F-685, F-695 and the long-wave emission showed a distinct increase upon cooling. For F-685 and F-695 the temperature dependence was similar to that earlier observed with spinach chloroplasts, for the long-wave emission it appeared to depend on the location of the emission bands, which was different for different species. All three bands were strongly quenched by quinones. These and other data suggest that the origin of these bands is the same as in higher plants, and that the fluorescence increase upon cooling can be explained by a lowering of the efficiency of energy transfer between chlorophyll molecules. It is concluded that at most a small percentage of the emission at 685 nm can be ascribed to allophycocyanin B, and that the efficiency of energy transfer between allophycocyanin B and chlorophyll a probably exceeds 99% both at 77 and 4 K. Experiments with isolated phycobilisomes suggest that energy transfer from allophycocyanin to allophycocyanin B occurs with an efficiency of about 90% at low temperature.

The effect of quenchers can be understood by the assumption that the quenching is caused by the formation of non-fluorescent traps in the bulk chlorophyll. Of three quinones tested, the strongest quenching was observed with dibromothymoquinone, which quenched F-685, F-695 and the long-wave emission approximately equally. Menadione and 1,4-naphthoquinone, however, preferentially quenched the long-wave bands, indicating a stronger interaction with Photosystem I than with Photosystem II chlorophylls.     

A comparative study of the fluorescence properties of the chlorosomal antenna of the green bacterium from the family Oscillochloridaceae and the members from two other families of green bacteria

The fluorescence properties of bacteriochlorophylls (BChl) of the chlorosomal light-harvesting antenna of Oscillochloris trichoides (strain DG-6) from a new family of green filamentous bacteria Oscillochloridaceae were investigated in comparison with green bacteria from two other families. A strong dependence of the fluorescence intensity of chlorosomal bacteriochlorophyll c of Osc. trichoides on the redox potential of medium was found, which previously was observed only in green sulfur bacteria. The presence of BChl a in chlorosomes did not appear in their absorption spectra but was visualized by fluorescence spectroscopy at 77 K. From the comparative analysis of fluorescence spectral data for the chlorosomal light-harvesting antenna of Osc. trichoides and similar spectral data for green bacteria from two other families, it was concluded that, in some fluorescence spectral features (spectral position of bacteriochlorophyll c/a fluorescence bands; shape and full width at half maximum fluorescence band of chlorosomal bacteriochlorophyll c; the Stokes shift value of bacteriochlorophyll c band; a high molar ratio of bacteriochlorophyll c : bacteriochlorophyll a in chlorosomes that makes the bacteriochlorophyll a fluorescence band unresolved at room temperature; and highly redox-dependent fluorescence intensity of chlorosomal bacteriochlorophyll c), Osc. trichoides chlorosomes are close to the chlorosomal antenna of Chlorobiaceae species.     

Electron paramagnetic resonance saturation studies of P-700 reaction center chlorophyll in plant photosynthesis

Electron paramagnetic resonance (EPR) power saturation and saturation recovery methods have been used to determine the spin lattice, T₁, and spin-spin, T₂, relaxation times of P-700⁺ reaction-center chlorophyll in Photosystem I of plant chloroplasts for 10 K T 100 K. T₁ was 200 μs at 100 K and increased to 900 μs at 10 K. T₂ was 40 ns at 40 K and increased to 100 ns at 10 K. T₁ for 40 K T 100 K is inversely proportional to temperature, which is evidence of a direct-lattice relaxation process. At T = 20 K, T₁ deviates from the 1/T dependence, indicating a cross relaxation process with an unidentified paramagnetic species. The individual effects of ascorbate and ferricyanide on T₁ of P-700⁺ were examined: T₁ of P-700⁺ was not affected by adding 10 mM ascorbate to digitonin-treated chloroplast fragments (D144 fragments). The P-700⁺ relaxation time in broken chloroplasts treated with 10 mM ferricyanide was 4-times shorter than in the untreated control at 40 K. Ferricyanide appears to be relaxing the P-700⁺ indirectly to the lattice by a cross-relaxation process. The possibility of dipolar-spin broadening of P-700⁺ due to either the iron-sulfur center A or plastocyanin was examined by determining the spin-packet linewidth for P-700⁺ when center A and plastocyanin were in either the reduced or oxidized states. Neither reduced center A nor oxidized plastocyanin was capable of broadening the spin-packet linewidth of the P-700⁺ signal. The absence of diplolar broadening indicates that both center A and plastocyanin are located at a distance at least 3.0 nm from the P-700⁺ reaction center chlorophyll. This evidence supports previous hypotheses that the electron donor and acceptor to P-700 are situated on opposite sides of the chloroplast membrane. It is also shown that the ratio of photo-oxidized P-700 to photoreduced centers A and B at low temperature is 2 : 1 if P-700 is monitored at a nonsaturating microwave power.     

Flash-induced absorption changes in Photosystem I,Radical pair or triplet state formation?

Absorption changes induced in chlorophyll protein (CP 1) particles by short laser flashes have been analyzed in order to decide whether a state lasting for a few microseconds at 21°C or 800 μs at 10 K corresponds to the biradical P-700⁺ ... A⁻₁ (A₁ being a chlorophyll a) or to a triplet state produced in a submicrosecond recombination of the preceding state. At 21°C the spectrum of the flash-induced ΔA (720–870 nm) presents a flat-topped band from 740 to 820 nm, clearly different from that of P-700⁺. A saturation curve (ΔA vs. laser energy), obtained with a 2 or 10 ns laser pulse, indicates that ΔA saturates at a value 2- or 3-times smaller than that expected on the basis of the chemical oxidation of P-700. At 21°C the size of flash-induced ΔA is slightly decreased (5–15%) when the sample is subjected to a 400 G magnetic field. The kinetics of decay are not affected; they are not affected either by the oxygen concentration. At 10 K the spectrum of the flash-induced ΔA has been measured between 650 and 1700 nm. Between 650 and 720 nm, the spectrum presents only one major negative peak at 702 nm; it is quite different from that due to the chemical oxidation of P-700 (which has additional peaks at 688 and 677 nm). Between 720 and 870 nm, the spectrum is identical to that obtained at 21°C. Above 870 nm, the spectrum includes a broad band around 1250 nm, which is absent in P-700⁺. A saturation curve leads to a maximum ΔA greater than that at 21°C and which is also greater with a 1 μs dye laser flash than with a 10 ns ruby laser flash. An analysis of the spectral data indicates that these do not fit correctly with the hypothesis of a contribution of P-700⁺ and of a chlorophyll a anion radical. They fit more closely with the hypothesis of a triplet state of P-700, a hypothesis which is discussed in relation to other experimental data.     

Energy transfer and bacteriochlorophyll fluorescence in purple bacteria at low temperature

Emission spectra of bacteriochlorophyll a fluorescence and absorption spectra of various purple bacteria were measured at temperatures between 295 and 4 K. For Rhodospirillum rubrum the relative yield of photochemistry was measured in the same temperature region. In agreement with earlier results, sharpening and shifts of absorption bands were observed upon cooling to 77 K. Below 77 K further sharpening occurred. In all species an absorption band was observed at 751-757 nm. The position of this band and its amplitude relative to the concentration of reaction centers indicate that this band is due to reaction center bacteriopheophytin. The main infrared absorption band of Rhodopseudomonas sphaeroides strain R26 is resolved in two bands at low temperature, which may suggest that there are two pigment-protein complexes in this species. Emission bands, like the absorption bands, shifted and sharpened upon cooling. The fluorescence yield remained constant or even decreased in some species between room temperature and 120 K, but showed an increased below 120 K. This increase was most pronounced in species, such as R. rubrum, which showed single banded emission spectra. In Chromatium vinosum three (835, 893 and 934 nm) and in Rps. sphaeroides two (888 and 909 nm) emission bands were observed at low temperature. The temperature dependence of the amplitudes of the short wavelength bands indicated the absence of a thermal equilibrium for the excitation energy distribution in C. vinosum and Rps. sphaeroides. In all species the increased in the yield was larger when all reaction centers were photochemically active than when the reaction centers were closed. In R. rubrum the increase in the fluorescence yield was accompanied by a decrease of the quantum yield of charge separation upon excitation of the antenna but not of the reaction center chlorophyll. Calculation of the F?rster resonance integral at various temperatures indicated that the increase in fluorescence yield and the decrease in the yield of photochemistry may be due to a decrease in the rate of energy transfer between antenna bacteriochlorophyll molecules. The energy transfer from carotenoids to bacteriochlorophyll was independent of the temperature in all species examined. The results are discussed in terms of existing models for energy transfer in the antenna pigment system.     

Pigment content and molar extinction coefficients of photochemical reaction centers from Rhodopseudomonas spheroides

Reaction center particles isolated from carotenoidless mutant Rhodopseudomonas spheroides were studied with the aim of determining the pigment composition and the molar extinction coefficients.

Two independent sets of measurements using a variety of methods show that a sample with A_{800 nm} = 1.00 contains 20.8 ± 0.8 μM tetrapyrrole and that the ratio of bacteriochlorophyll to bacteriopheophytin is 2:1.

Measurements were made of the absorption changes attending the oxidation of cytochrome c coupled to reduction of the photooxidized primary electron donor in reaction centers, using laser flash excitation. The ratio of the absorption change at 865 nm (due to the bleaching of P870) to that at 550 nm (oxidation of cytochrome) was found to be 5.77.

These results, combined with other data, yield a pigment composition of 4 bacteriochlorophyll and 2 bacteriopheophytin molecules in a reaction center. Based on this choice, extinction coefficients are determined for the 802- and 865-nm bands: _{802 nm} = 288 (± 14) mM⁻¹ · cm⁻¹ and _{865 nm} = 128 (± 6) mM⁻¹ · cm⁻¹. For reversible bleaching of the 865-nm band, Δ^{red - ox}_865nm = 112 (± 6) mM⁻¹ · cm⁻¹ (referred to the molarity of reaction centers). Earlier reported values of photochemical quantum efficiency are recomputed, and the revised values are shown to be compatible with those obtained from measurements of fluorescence transients.     

Temperature-dependent regulation of d-cis-[H]diltiazem binding to Ca channels by 1,4-dihydropyridine channel agonists and antagonists

The binding of the Ca²⁺-channel blocker d-cis-[³H]diltiazem to guinea pig skeletal muscle microsomes is temperature-dependent. At 2°C the K_D is 39 nM and B_max is 11 pmol/mg protein. The binding is fully reversible (K₋₁ = 0.02 min⁻¹). The binding sites discriminate between the diastereoisomers 1- and d-cis-diltiazem, recognize verapamil, gallopamil and tiapamil, and are sensitive to La³⁺-inhibition. At 30°C the K_D is 37 nM and the B_max is 2.9 pmol/mg protein. D-cis-diltiazem-labelling is regulated by the 1,4-dihydropyridine Ca²⁺-channel blockers and a novel Ca²⁺-channel activator in a temperature-dependent manner. At 30°C an enhancement of d-cis-diltiazem binding by the channel blockers is observed. This is attributed to a B_max increase. EC₅₀-values for enhancement and the maximal enhancement differ for the individual 1,4-dihydropyridines. At 2°C 1,4-dihydropyridines inhibit d-cis-[³H]diltiazem binding. This is attributed to a B_max decrease. We have directly labelled one of the drug receptor sites within the Ca²⁺-channel which can allosterically interact with the 1,4-dihydropyridine binding sites.     

Molecular structures and some properties of tris(2-aminoethyl) amine cobalt(III) complexes with thiocarboxylato-O,S such as 3-mercaptopropionato, 2-mercaptoacetato and their derivatives

Cobalt(III) complexes with a thiolate or thioether ligand, t-[Co(mp)(tren)]⁺ (2), t-[Co(mtp)(tren)]²⁺ (1Me) and t-[Co(mta)(tren)]²⁺ (2Me), (mp = 3-mercaptopropionate, MA = 3-(methylthio)propionate and MTA = 2-(methylthio)acetate) have been prepared in aqueous solutions. The crystal structures of 1, 2, 1Me and 2Me were determined by X-ray diffraction methods. The crystal data are as follows, t-[Co(mp)(tren)]ClO₄ (1CIO₄): monoclinic, P2₁/n, A = 10.877(8), B = 11.570(4), c = 12.173(7) Å, β = 92.20(5)°, V = 1531(1) ų, Z = 4 and R = 0.060; t-[Co(ma)(tren)]Cl·3H₂O (2Cl·3H₂O): monoclinic, P2₁/n, a = 7.7688(8), B = 27.128(2), C = 7.858(1) Å, β = 100.63(1)°, V = 1627.7(3) ų, Z = 4 and R = 0.066; (+)₄₆₅^CD-t-[Co(mtp)(tren)](ClO₄)₂ ((+)₄₆₅^CD-1Me(ClO₄)₂): orthorhombic, P2₁2₁2₁, A = 10.6610(7), B = 11.746(1), C = 15.555(1) Å, V = 1947.9(3) ų, Z = 4 and R = 0.068; (+)₄₆₅^CD-t-[Co(mta)(tren)](ClO₄)₂ ((+)₄₆₅^CD-2Me(ClO₄)₂): orthorhombic, P2₁2₁2₁, a = 10.564(1), B = 11.375(1), C = 15.434(2) Å, V = 1854.7(4) ų, Z = 4 and R = 0.047. All central Co(III) atoms have approximately octahedral geometry, coordinated by four N, one O, and one S atoms. All of the complexes are only isomer, of which the sulfur atom in the didentate-O,S ligands are located at the trans position to the tertiary amine nitrogen atom of tren. 1 and 1Me contain six-membered chelate ring, and 2 and 2Me do five-membered chelate ring in the didentate ligand. The chirality of the asymmetric sulfur donor atom in (+)₄₆₅^CD-1Me is the S configuration and that in (+)₄₆₅^CD-2Me is the R one. The ¹H NMR, ¹³C NMR and electronic absorption spectral behaviors and electrochemical properties of the present complexes are discussed in relation to their stereochemistries.     

Optical and structural properties of chlorosomes of the photosynthetic green sulfur bacterium Chlorobium limicola

Isolated chlorosomes of the photosynthetic green sulfur bacterium Chorobium limicola upon cooling to 4 K showed, in addition to the near-infrared absorption band at 753 nm due to bacteriochlorophyll c, a weak band near 800 nm that could be attributed to bacteriochlorophyll a. The emission spectrum showed bands of bacteriochlorophyll c and a at 788 and 828 nm, respectively. The fluorescence excitation spectrum indicated a high efficiency of energy transfer from bacteriochlorophyll c to bacteriochlorophyll a. When all bacteriochlorophyll c absorption had been lost upon storage, no appreciable change in the optical properties of the bacteriochlorophyll a contained in these ‘depleted chlorosomes’ was observed. The fluorescence and absorption spectra of the chlorosomal bacteriochlorophyll a were clearly different from those of the soluble bacteriochlorophyll a protein present in these bacteria. The results provide strong evidence that bacteriochlorophyll a, although present in a small amount, is an integral constituent of the chlorosome. It presumably functions in the transfer of energy from the chlorosome to the photosynthetic membrane; its spectral properties and the orientation of its near-infrared optical transitions as determined by linear dichroism are such as to favor this energy transfer.     

Energy transfer in the B800-850-carotenoid light-harvesting complex of various mutants of Rhodopseudomonas sphaeroides and of Rhodopseudomonas capsulata

Emission and absorption spectra in the temperature range 4–300 K have been obtained for bacteriochlorophyll light-harvesting complexes (B800–850 complexes) from several mutants of Rhodopseudomonas sphaeroides and a nonphotosynthetic mutant of Rhodopseudomonas capsulata. The energy-transfer properties of these complexes were remarkably similar despite differences in carotenoid composition. Between 300 and 200 K the excitation densities in B800 and B850 are in thermal equilibrium, indicating rapid energy transfer from B800 to B850 and vice versa. The temperature dependence of the ratio of the B800 and B850 emission yields allows the determination of the ratio of the number of B800 and B850 molecules in the complex which is close to 0.5. Below 200 K thermal equilibrium no longer exists. At 4–100 K the B800 emission yield increases with decreasing temperature and becomes dependent on the wavelength of excitation. From the B800 emission yield at 4 K the B800–850 dipole-dipole distance was calculated to be equal to or smaller than 21 Å for all B800–850 complexes. Excitation spectra for B800 and B850 emission show that the overall energy-transfer efficiencies from carotenoid and B800 to B850 are greater than 90% at all temperatures. At 4 K the carotenoid transfers its excitation energy preferentially to B850. Experiments with chromatophores indicated that the energy-transfer properties of the B800–850 complexes were not modified by the isolation procedures.     

Fluorescence emission spectra of chloroplasts and subchloroplast preparations at low temperature.

A study was made of the chlorophyll fluorescence spectra between 100 and 4.2 K of chloroplasts of various species of higher plants (wild strains and chlorophyll b mutants) and of subchloroplast particles enriched in Photosystem I or II. The chloroplast spectra showed the well known emission bands at about 685, 695 and 715--740 nm; the System I and II particles showed bands at about 675, 695 and 720 nm and near 685 nm, respectively. The effect of temperature lowering was similar for chloroplasts and subchloroplast particles; for the long wave bands an increase in intensity occurred mainly between 100 and 50 K, whereas the bands near 685 nm showed a considerable increase in the region of 50--4.2 K. In addition to this we observed an emission band near 680 nm in chloroplasts, the amplitude of which was less dependent on temperature. The band was missing in barley mutant no. 2, which lacks the light-harvesting chlorophyll a/b-protein complex. At 4.7 K the spectra of the variable fluorescence (Fv) consisted mainly of the emission bands near 685 and 695 nm, and showed only little far-red emission and no contribution of the band at 680 nm. From these and other data it is concluded that the emission at 680 nm is due to the light-harvesting complex, and that the bands at 685 and 695 nm are emitted by the System II pigment-protein complex. At 4.2 K, energy transfer from System II to the light-harvesting complex is blocked, but not from the light-harvesting to the System I and System II complexes. The fluorescence yield of the chlorophyll species emitting at 685 nm appears to be directly modulated by the trapping state of the reaction center.     

Bacteriochlorophyll a-types in chromatophore and subchromatophore preparations from Rhodopseudomonas sphaeroides.

Comparison of absorption and circular dichroism (CD) spectra in the near infrared region was made with chromatophore and subchromatophore preparations obtained from Rhodopseudomonas sphaeroides. The 850 nm absorption band had a positive correlation with the 850 nm and 870 nm CD bands. The 800 nm and 870 nm absorption bands seemed not to correlate with any CD bands. Lipid contents in chromatophores and subchromatophores were measured. Lipids in membranes seemed to contribute to the appearance of the 870 nm absorption band, but not to that of the 800 nm and 850 nm absorption bands. The time courses of absorbance changes were compared at 800, 850, and 870 nm in detergent-treated chromatophores. Relative changes of absorbances differed from one another. The present results suggest that the three absorption bands are due to three different bacteriochlorophyll a-types and the 850 nm absorption band originates from exciton-coupling of bacteriochlorophyll a.     

Band Structure and Local Dynamics of Excitons in Bacterial Light-harvesting Complexes Revealed by Spectrally Selective Spectroscopy

Hole-burned absorption and line-narrowed fluorescence spectra are studied at 5 K in wild type and mutant LH1 and LH2 antenna preparations from the photosynthetic purple bacterium Rhodobacter sphaeroides. Evidence was found in all samples, even in intact membranes, of the presence of a broad distribution of bacteriochlorophyll species that are unable to communicate energy between each other and to the exciton states of functional antenna complexes. The distribution maximum of these localized species determined by zero phonon hole action spectroscopy is at 783.5 nm in purified LH1 complexes and at 786.8 nm in B850-only mutant LH2 complexes. A well-resolved peak at 807 nm in LH1 complexes is assigned to the exciton band structure of functional core antenna complexes. Similar structure in LH2 complexes overlaps with the distribution of localized species. Off-diagonal (structural) disorder may be responsible for this exciton band structure. Our data also imply that pair-wise inter-chlorophyll couplings determine the resonance fluorescence lineshape of excitonic polarons.     

Structure, physical, chemical and photophysical properties of Pt(bph) (CO)2, where bph is the biphenyl dianion

The complex Pt(bph) (CO)₂ crystallizes in the space group Cmcm with a = 18.647(6), B = 9.566(2) and C = 6.4060(5) Å. The geometry of the molecule is slightly distorted from square planar with a Pt---C(CO) bond distance of 1.98(2) Å and a Pt---C(bph) bond distance of 2.04(2) Å. The Pt(bph)(CO)₂ complex serves as a precursor for the preparation of a wide variety of Pt(bph)X₂ complexes, where X = monodentate ligands such as acetonitrile, pyridine, etc., and X₂ = bidentate ligands such as bypyridine, 1,10-phenanthroline, etc. In the solid state, the complex exhibits a green color, but when ground with an alkali metal salt turns deep blue to purple. In CH₂Cl₂, the color disappears but optical transitions are observed at 271 nm (2.7 × 10⁴ M⁻¹ cm⁻¹), 303 nm (1.1 × 10⁴ M⁻¹ cm⁻¹) and 330 nm (5.5 × 10³ M⁻¹ cm⁻¹). The complex is a weak emitter exhibiting a structured spectrum in CH₂Cl₂ at r.t. with maxima located at 562 and 594 nm and an emission lifetime of 3.1 μs when excited at 337 nm.     

Absorbance and fluorescence properties of the bacteriochlorophyll a reaction center complex and bacteriochlorophyll a protein in green bacteria

Absorbance, emission and excitation spectra were measured at both room and liquid-nitrogen temperatures for a photochemically active bacteriochlorophyll a reaction center complex and a bacteriochlorophyll a protein isolated from Chlorobium limicola and Chlorobium thiosulfatophilum. The low-temperature absorbance spectrum for the complex has a band centered at 833 nm, which is not seen in the spectrum of the bacteriochlorophyll a protein. We attribute this difference to a modification of the bacteriochlorophyll a protein in the active complex. The room-temperature fluorescence spectra for the bacteriochlorophyll a protein and the complex are similar, as are those measured at low temperatures. The 833-nm component of the low-temperature absorbance spectrum of the complex is relatively nonfluorescent.