Effects of light quality on chlorophyll-forms Ca 684, Ca 690 and Ca 699 of the diatom Phaeodactylum tricornutum

Colored light modifies the relative concentration of chlorophyll-forms of the diatom Phaeodactylum tricornutum compared to white-light control. No change in the ratio carotenoids/chlorophylls was observed after 4 days exposure to green light (max: 530 nm), blue light (max: 470 nm) or red light ( > 650 nm) of same intensity.However, the absorption spectra were modified, the content in Ca 684, Ca 690, Ca 699 forms increased in red and green light cultures and photosynthetic unit size of PS II decreased by 30% in green and blue light cultures.Fluorescence emission and fluorescence excitation spectra according to the Butler and Kitajima method (1975) were carried out for each culture. Ca 669 form was predominant in the two photosystems. The newly appeared far red forms fluoresce at 715 nm like PS I forms.We conclude that these new forms originated in a rearrangement of PS II forms. They do not transmit excitation energy to reaction center of PS I and are disconnected from the other chlorophyll-forms of the photosynthetic antennae.Abbreviations ABS absorption - Ca chlorophyll-complex - chla chlorophyll a - chl c chlorophyll c - chl t total chlorophylls - D.C.M.U. 3-(3, 4 dichlorophenyl) 1-diméthyl-urea - d^v division - F fluorescence - PS I and PS II photosystem I and photosystem II     

On the differences of molecular aggregates structure with long wave fluorescence in the photosystems I and II]

Galactolipase and protenase action on the low temperature fluorescence spectra of light chloroplast fragments obtained from grana or intergrana thylakoids and grana thylakoids system before and after isolation photosystem I particles have been studied. Identical hydrolytic enzymes action in the two type photosystem I particles have been studied. Identical hydrolytic enzymes action in the two type photosystem I particles were observed. Grana thylakoids system after removing photosystem I particles contained photosystem II in the most purified form. These measurements results confirmed our previous suggestion that the band at 735 nm in the low temperature fluorescence spectra of light and heavy fragments belongs to the different native chlorophyll a aggregates.     

Spectral anisotropy of chloroplasts, subchloroplast particles and pigment-protein complexes

Anisotropic properties of pea chloroplasts, subchloroplast fragments (photosystem 1 particles and pigment-protein complexes) and the blue-green algae oriented in polyacrylamide gel were investigated. It was shown that linear dichroism spectra of chloroplasts are the superposition of the corresponding spectra for the main light harvesting complex (HMLC) and P 700 chlorophyll a--protein complex (CP 1). Anisotropic properties of the photosystem 1 particles and blue-green algae are mainly caused by CP 1 anisotropy. Qy-transition moments tend to perpendicular orientation to the membrane plane for the Chl. b 649, Chl. a 660 and parallel orientation--for Chl. b 654, Chl. a 682. The degree of Qy-transition moments parallel orientation is higher for the longwave forms (Chl. a 690, Chl. a 702, Chl. a 712), than for the shortwave ones and coincides with this degree for the reaction centre pigment P 700 transition moment. It is suggested that the specific orientation of the pigment-protein complexes in the chloroplast membrane is important for the regulation of the spillover between two photosystems.     

毕氏海蓬子光系统Ⅱ颗粒的分离与鉴定

采用去污剂TritonX-100增溶类囊体膜和高速离心的方法,首次分离和纯化了毕氏海蓬子的光系统Ⅱ（photosystemⅡ,PSⅡ）颗粒,通过光谱学和SDS-PAGE对其进行鉴定并与类囊体膜进行比较。室温吸收光谱结果表明,PSⅡ颗粒在蓝区的叶绿素（chlorophyll,ChOb和胡萝卜素类吸收峰为485nm,在红区的Ch1b吸收峰为655nm,这两个峰值均低于类囊体膜中的。77K荧光发射光谱结果表明,提取的PSⅡ颗粒基本不含光系统Ⅰ（photosystemⅠ,PSI）的低温荧光反射峰737nm。77K荧光激发光谱结果显示,海蓬子PSⅡ颗粒在470-485am之间的Ch1b 和胡萝卜素类的荧光发射峰明显低于类囊体膜的。这说明在PSⅡ中大部分的PSI已被除去。电泳结果显示,海蓬子PSⅡ颗粒缺少PSI反应中心蛋白质亚基PsaA和PsaB,这说明提取到的PSⅡ纯度较高,这为进一步研究毕氏海蓬子PSⅡ的结构与功能奠定基础。     

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.     

Analyses of absorption and fluorescence spectra of water-soluble chlorophyll proteins, pigment system II particles and chlorophyll a in diethylether solution by the curve-fitting method.

Absorption and fluorescence spectra in the red region of water-soluble chlorophyll proteins, Lepidium CP661, CP663 and Brassica CP673, pigment System II particles of spinach chloroplasts and chlorophyll a in diethylether solution at 25 degrees C were analyzed by the curve-fitting method (French, C.S., Brown, J.S. and Lawrence, M.C. (1972) Plant Physiol 49, 421--429). It was found that each of the chlorophyll forms of the chlorophyll proteins and the pigment System II particles had a corresponding fluorescence band with the Stokes shift ranging from 0.6 to 4.0 nm. The absorption spectrum of chlorophyll a in diethylether solution was analyzed to one major band with a peak at 660.5 nm and some minor bands, while the fluorescence spectrum was analyzed to one major band with a peak at 664.9 nm and some minor bands. A mirror image was clearly demonstrated between the resolved spectra of absorption and fluorescence. The absorption spectrum of Lepidium CP661 was composed of a chlorophyll b form with a peak at 652.8 nm and two chlorophyll a forms with peaks at 662.6 and 671.9 nm. The fluorescence spectrum was analyzed to five component bands. Three of them with peaks at 654.8, 664.6 and 674.6 nm were attributed to emissions of the three chlorophyll forms with the Stokes shift of 2.0--2.7 nm. The absorption spectrum of Brassica CP673 had a chlorophyll b form with a peak at 653.7 nm and four chlorophyll a forms with peaks at 662.7, 671.3, 676.9 and 684.2 nm. The fluorescence spectrum was resolved into seven component bands. Four of them with peaks at 666.7, 673.1, 677.5 and 686.2 nm corresponded to the four chlorophyll a forms with the Stokes shift of 0.6--4.0 nm. The absorption spectrum of the pigment System II particles had a chlorophyll b form with a peak at 652.4 nm and three chlorophyll a forms with peaks at 662.9, 672.1 and 681.6 nm. The fluorescence spectrum was analyzed to four major component bands with peaks at 674.1, 682.8, 692.0 and 706.7 nm and some minor bands. The former two bands corresponded to the chlorophyll a forms with peaks at 672.1 and 681.6 nm with the Stokes shift of 2.0 and 1.2 nm, respectively. Absorption spectra at 25 degrees C and at --196 degrees C of the water-soluble chlorophyll proteins were compared by the curve-fitting methods. The component bands at --196 degrees C were blue-shifted by 0.8--4.1 nm and narrower in half widths as compared to those at 25 degrees C.     

Photoinduced changes in adsorption at 800 nm related to photosystem I functioning]

The spectra and kinetics of light-induced absorbance changes in the near-infrared region of subchloroplast fragments enriched by P700 were studied. An increase in absorbancy within the region of 725--900 nm upon illumination was characterized by a maximum around 810 nm and by "shoulders" around 760 and 870 nm. Similar effects of thermal inactivation and low temperatures on the duration of dark recovery of light-induced absorbance changes at 700 nm and within the region of 725--900 nm suggest that the absorbance changes in the near-infrared region are due to photooxidation of P700. The values of P700 differential extinction coefficients at 810 nm are 8,2.10(3) M-1.cm-1 for digitonin fragments and 7,7.10(3) M-1.cm-1 for fragments prepared with the use of diethyl ester. It was shown that the value of midpoint oxidation-reduction potential measured for the absorbance changes at 810 nm (+492 mv) is higher than that measured at 700 nm (+475 mv).     

Organization of the Marginal Regions of Pea Granal Thylakoids

Thylakoids of pea chloroplasts isolated from plants grown during various time intervals from June to August were subjected to fragmentation. Using a modified procedure, a fraction of larger particles was separated from those previously considered as fragments of intergranal thylakoids. The particles of the fraction isolated were identified as fragments of marginal regions of granal thylakoids (margins). The relative yield of these fragments depended on the time interval of plant growth. Two types of low-temperature fluorescence spectra corresponding to a high and low yield of the fraction were detected. The characteristics of the first one were a high fluorescence intensity in the short-wave region and the presence of bands with maxima at 687 and 696 nm emitted by photosystem II (PSII). The ratio of PSII to PSI complexes (PSII/PSI) in the fractions characterized by a low and high yield varied from 1 to 5. The analysis of excitation spectra of long-wave fluorescence of PSI showed that PSI complexes in the margin fragments obtained at a low fraction yield were depleted in chlorophyll forms with a 682-nm absorption maximum and enriched in those with a 668-nm maximum. Since an increase in the yield of the margin-fragment fraction is due to an increased unstacking of granal thylakoids, the differences in the characteristics of fragments obtained with a low and a high yield reflect the changes in the composition of granal thylakoids in the direction from the margin to the centrum, that is, a decrease in the relative content of PSI complexes and alterations in the composition and size of its light-harvesting antenna. The consistency between the data obtained and the present view concerning the different functions of PSI located in different thylakoid regions is discussed.     

A single step separation of PS 1, PS 2 and chlorophyll-antenna particles from spinach chloroplasts

After solubilization of photosynthetic membranes by digitonin, three main protein pigment complexes were isolated by electrophoresis with deoxycholate as detergent.The band with the slowest mobility, fraction 1, had PS 1 activity and was devoid of PS 2 activity. This fraction was four times enriched in P700 when compared with chloroplasts. Fraction 1 had little chl b, a long wavelength absorption maximum in the red, a maximum of low temperature emission fluorescence at 730nm, and a circular dichroism spectrum characteristic of PS 1 enriched fraction.Fraction 2 exhibited a PS 2 activity and no PS 1 activity. It was enriched five times in PS 2 reaction centre and had little chl b and carotenoids. The absorption maximum was at 674 nm and the low temperature fluorescence emission maximum was at 700 nm. Fraction 2 might be useful PS 2 enriched particle because of the great stability of this fraction with regard to photochemical activity and also rapidity and simplicity of its preparation.Fraction 3, which had the fastest migration, was devoid of photochemical activities; It was rich in chl b and had the fluorescence and the circular dichroism spectrum characteristic of an antenna complex.Abbreviations PS 1 (2) photosystem 1 (2) - chl chlorophyll - car carotenoid - Q primary plastoquinone electron acceptor - P700 primary electron donor of PS 1 - P680 primary electron donor of PS 2 - K₃Fe(CN)₆ potassium ferricyanide - DCMU dichlorophenyldimethylurea - DCPIP dichlorophenolindophenol - DPC diphenyl-carbazide     

Iron Deficiency in the Blue-Green Alga Anacystis nidulans: Fluorescence and Absorption Spectra Recorded at 77°K

Low-temperature (77°K) fluorescence and absorption spectra have been determined for whole cells and photosystem I particles of Anacystis nidulans grown in iron-supplied or iron-deficient inorganic media. Iron deficiency induces a decrease of F720 relative to F685 and F695 in the fluorescence spectra of both whole cells and photosystem I particles. This change is correlated to a reduction of preferentially the long wavelength absorbing fraction of chlorophyll a. The relative fluorescence intensity at 755 nm is increased by iron deficiency. No significant effects of culture-age are found in the ratio between the three fluorescence bands (F685: F695: F720) of iron-supplied A. nidulans.     

Excitation dynamics and heterogeneity of energy equilibration in the core antenna of photosystem I from the cyanobacterium Synechocystis sp. PCC 6803

Energy equilibration in the photosystem I core antenna from the cyanobacterium Synechocystis sp. PCC 6803 was studied using femtosecond transient absorption spectroscopy at 298 K. The photosystem I core particles were excited at 660, 693, and 710 nm with 150 fs spectrally narrow laser pulses (fwhm = 5 nm). Global analysis revealed three kinetic processes in the core antenna with lifetimes of 250-500 fs, 1.5-2.5 ps, and 20-30 ps. The first two components represent strongly excitation wavelength-dependent energy equilibration processes while the 20-30 ps phase reflects the trapping of energy by the reaction center. Excitation into the blue and red edge of the absorption band induces downhill and uphill energy flows, respectively, between different chlorophyll a spectral forms of the core. Excitation at 660 nm induces a 500 fs downhill equilibration process within the bulk of antenna while the selective excitation of long-wavelength-absorbing chlorophylls at 710 nm results in a 380 fs uphill energy transfer to the chlorophylls absorbing around 695-700 nm, presumably reaction center pigments. The 1.5-2.5 ps phases of downhill and uphill energy transfer are largely equivalent but opposite in direction, indicating energy equilibration between bulk antenna chlorophylls at 685 nm and spectral forms absorbing below 700 nm. Transient absorption spectra with excitation at 693 nm exhibit spectral evolution within approximately 2 ps of uphill energy transfer to major spectral forms at 680 nm and downhill energy transfer to red pigments at 705 nm. The 20-30 ps trapping component and P(700) photooxidation spectra derived from data on the 100 ps scale are largely excitation wavelength independent. An additional decay component of red pigments at 710 nm can be induced either by selective excitation of red pigments or by decreasing the temperature to 264 K. This component may represent one of the phases of energy transfer from inhomogeneously broadened red pigments to P(700). The data are discussed based on the available structural model of the photosystem I reaction center and its core antenna.     

Electronic spectra of PS I mutants: the peripheral subunits do not bind red chlorophylls in Synechocystis sp. PCC 6803

Steady-state fluorescence and absorption spectra have been obtained in the Qy spectral region (690-780 nm and 600-750 nm, respectively) for several subunit-deficient photosystem I mutants from the cyanobacterium Synechocystis sp. PCC 6803. The 77 K fluorescence spectra of the wild-type and subunit-deficient mutant photosystem I particles are all very similar, peaking at approximately 720 nm with essentially the same excitation spectrum. Because emission from far-red chlorophylls absorbing near 708 nm dominates low-temperature fluorescence in Synechocystis sp., these pigments are not coordinated to any the subunits PsaF, Psa I, PsaJ, PsaK, PsaL, or psaM. The room temperature (wild-type-mutant) absorption difference spectra for trimeric mutants lacking the PsaF/J, PsaK, and PsaM subunits suggest that these mutants are deficient in core antenna chlorophylls (Chls) absorbing near 685, 670, 675, and 700 nm, respectively. The absorption difference spectrum for the PsaF/J/I/L-deficient photosystem I complexes at 5 K reveals considerably more structure than the room-temperature spectrum. The integrated absorbance difference spectra (when normalized to the total PS I Qy spectral area) are comparable to the fractions of Chls bound by the respective (groups of) subunits, according to the 4-A density map of PS I from Synechococcus elongatus. The spectrum of the monomeric PsaL-deficient mutant suggests that this subunit may bind pigments absorbing near 700 nm.     

BIO-OPTICAL CHARACTERISTICS AND PHOTOADAPTIVE RESPONSES IN THE TOXIC AND BLOOM-FORMING DINOFLAGELLATES GYRODINIUM AUREOLUM,GYMNODINIUM GALATHEANUM,AND TWO STRAINS OF PROROCENTRUM MINIMUM1

Photoadaptive responses in the toxic and bloom-forming dinoflagellates Gyrodinium aureolum Hulbert, Gymnodinium galatheanum Braarud, and two strains of Prorocentrum minimum (Pavillard)Schiller were evaluated with respect to pigment composition, light-harvesting characteristics, carbon and nitrogen contents, and growth rates in shade- and light-adapted cells. The two former species were grown at scalar irradiances of 30 and 170 μmol · m ^?2 at a 12-h daylength at 20° C. The two strains of P. minimum were grown at 35 and 500 μmol. m^?2· s^?1 at a 2-h daylength at 20° C. For the first time, chlorophyll (chl) c₃, characteristic of several bloom-forming prymnesiophytes, was detected in G. aureolum and G. galatheanum. Photoadaptional status affected the pigment composition strongly, and the interpretation of the variation depended on whether the pigment composition was normalized per cell, carbon, or chl a. Species-specific and photoadaptional differences in chl a-specific absorption (°a_c, 400–700 nm) and chl a-normalized fluorescence excitation spectra of photosystem II fluorescence with or without addition of DCMU (°F and °F_DCMU 400–700 nm) were evident. Gyrodinium aureolum and G. galatheanum exhibited in vivo spectral characteristics similar to chl c₃-containing prymnesiophytes in accordance with their similar pigmentation. Prorocentrum minimum had in vivo absorption and fluorescence characteristics typical for peridinin-containing dinoflagellates. Species-specific differences in in vivo absorption were also observed as a function of package effect vs. growth irradiance. This effect could be explained by differences in intracellular pigment content, cell size/shape, and chloroplast morphology/numbers. Light- and shade-adapted cells of P. minimum contained 43 and 17% of photoprotective carotenoids (diadino + diatoxanthin) relative to chl a, respectively. The photoprotective function of these carotenoids was clearly observed as a reduction in °F and °F ^DCMU at 400–540 nm compared to °ac in light-adapted cells of P. minimum. Spectrally weighted light absorption (normalized to chl a and carbon, 400–700 nm) varied with species and growth conditions. The use of quantum-corrected and normalized fluorescence excitation spectra with or without DCMU-treated cells to estimate photosynthetically usable light is discussed. The usefulness of in vitro absorption and fluorescence excitation spectra for estimation of the degradation status of chl a and the ratio of chl a to total pigments is also discussed.     

Photoreduction of 2,6-dichlorophenolindophenol by diphenylcarbazide: a photosystem 2 reaction catalyzed by tris-washed chloroplasts and subchloroplast fragments

The use of diphenylcarbazide as an electron donor coupled to the photoreduction of 2,6-dichlorophenolindophenol by tris-washed chloroplasts or subchloroplast fragments provides a simple and sensitive assay for photosystem 2 of chloroplasts. By varying the concentration of tris buffer at pH 8.0 during an incubation period it is shown that the destruction of oxygen evolution activity is accompanied by a corresponding emergence of an ability to photooxidize diphenylcarbazide, as evidenced by absorbance changes due to diphenylcarbazide at 300 nm. The temperature-sensitive oxidation of diphenylcarbazide is inhibited by DCMU and by high ionic strengths. This activity appears to measure the primary photochemical reaction of photosystem 2.     

Selective Formation of Photosystem 1 under Illumination at Low Intensity

Analyses of chlorophylls a and b and P700 in the wheat leaves grown for 8 days under illumination with white light at different intensities suggested selective formation of photosystem 1 of the photosynthesis at low light intensities. This was confirmed for the two types of chloroplasts isolated from leaves grown at light intensities of 1.1 and 240 μ W/cm², respectively, by measuring their pigment compositions, activities of photosystems 1 and 2, and absorption and fluorescence spectra. The chloroplasts developed at the low intensity showed properties only of photosystem 1 while those developed at the high intensity showed properties of both photosystems 1 and 2. Only photosystem 1 particles were obtained by fractionation of low intensity chloroplasts by treatment with digitonin followed by centrifugation, while high intensity chloroplasts could be fractionated into photosystem-1 and photosystem-2 particles. When the leaves grown at low light intensity were illuminated with strong light, photosystem 2 was developed. The fluorescence emission spectrum of low intensity chloroplasts at 77°K showed two peaks at 685 and 734 nm, and the spectrum of high intensity chloroplasts showed three peaks at 685, 697 and 740 nm.     

Triton X-100对70℃处理后光系统Ⅰ颗粒耗氧速率的影响

比较了70℃10min处理前后和加与不加Triton X-100时光系统Ⅰ颗粒的耗氧速率、荧光光谱和吸收光谱等.70℃处理后光系统Ⅰ颗粒的耗氧速率明显降低,Triton X-100可以恢复其耗氧速率.在Triton X-100存在时,光系统Ⅰ颗粒耗氧速率的急剧上升是光系统Ⅰ核心复合物和捕光色素蛋白复合体Ⅰ分离后产生的单线态氧引起的.     

Interaction of phycobilisomes with photosystem II dimers and photosystem I monomers and trimers in the cyanobacterium Spirulina platensis.

Distribution of phycobilisomes between photosystem I (PSI) and photosystem II (PSII) complexes in the cyanobacterium Spirulina platensis has been studied by analysis of the action spectra of H2 and O2 photoevolution and by analysis of the 77 K fluorescence excitation and emission spectra of the photosystems. PSI monomers and trimers were spectrally discriminated in the cell by the unique 760 nm low-temperature fluorescence, emitted by the trimers under reductive conditions. The phycobilisome-specific 625 nm peak was observed in the action spectra of both PSI and PSII, as well as in the 77 K fluorescence excitation spectra for chlorophyll emission at 695 nm (PSII), 730 nm (PSI monomers), and 760 nm (PSI trimers). The contributions of phycobilisomes to the absorption, action, and excitation spectra were derived from the in vivo absorption coefficients of phycobiliproteins and of chlorophyll. Analyzing the sum of PSI and PSII action spectra against the absorption spectrum and estimating the P700:P680 reaction center ratio of 5.7 in Spirulina, we calculated that PSII contained only 5% of the total chlorophyll, while PSI carried the greatest part, about 95%. Quantitative analysis of the obtained data showed that about 20% of phycobilisomes in Spirulina cells are bound to PSII, while 60% of phycobilisomes transfer the energy to PSI trimers, and the remaining 20% are associated with PSI monomers. A relevant model of organization of phycobilisomes and chlorophyll pigment-protein complexes in Spirulina is proposed. It is suggested that phycobilisomes are connected with PSII dimers, PSI trimers, and coupled PSI monomers.     

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 lightharvesting chlorophyll a/b-protein complex. At 4.7 K the spectra of the variable fluorescence (F_v) 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 emittting at 685 nm appears to be directly modulated by the trapping state of the reaction center.     

The photochemical trapping rate from red spectral states in PSI-LHCI is determined by thermal activation of energy transfer to bulk chlorophylls

The average fluorescence decay lifetimes, due to reaction centre photochemical trapping, were calculated for wavelengths in the 690- to 770-nm interval from the published fluorescence decay-associated emission spectra for Photosystem I (PSI)-light-harvesting complex of Photosystem I (LHCI) [Biochemistry 39 (2000) 6341] at 280 and 170 K. For 280 K, the overall trapping time at 690 nm is 81 ps and increases with wavelength to reach 103 ps at 770 nm. For 170 K, the 690-nm value is 115 ps, increasing to 458 ps at 770 nm. This underlines the presence of kinetically limiting processes in the PSI antenna (diffusion limited). The explanation of these nonconstant values for the overall trapping time band is sought in terms of thermally activated transfer from the red absorbing states to the "bulk" acceptor chlorophyll (chl) states in the framework of the Arrhenius-Eyring theory. It is shown that the wavelength-dependent "activation energies" come out in the range between 1.35 and 2.7 kcal mol(-1), increasing with the emission wavelength within the interval 710-770 nm. These values are in good agreement with the Arrhenius activation energy determined for the steady-state fluorescence yield over the range 130-280 K for PSI-LHCI. We conclude that the variable trapping time in PSI-LHCI can be accounted for entirely by thermally activated transfer from the low-energy chl states to the bulk acceptor states and therefore that the position of the various red states in the PSI antenna seems not to be of significant importance. The analysis shows that the bulk antenna acceptor states are on the low-energy side of the bulk antenna absorption band.     

Changes of the antenna of photosystem I induced by short-term heating

Changes in low-temperature fluorescence spectra of pea chloroplasts induced by the short-term heating were studied. Excitation spectra of the long-wavelength fluorescence were studied as well. Heating was carried out at 45°C for 5 min in the darkness or in the presence of white light sourced with intensities of 260 or 1400 μmol/m² s. All variants of heating decreased the intensity of the long-wavelength fluorescence band. The integral of the excitation spectrum decreased after the exposure to heating in the darkness and increased after the exposure to heating in the presence of light. The observed changes in most intensive components — 726, 729 and 731 nm — of the long-wavelength fluorescence band, induced by various modes of heating, were similar. The changes in the fourth intensive component at 735 nm were different. Twenty-five components were found in the fine structure of the excitation spectrum of the long-wavelength fluorescence. Positions of most of peaks corresponded to the absorption peaks of Lhca proteins. Heat-induced changes in the excitation spectrum in the regions corresponding to the absorption of chl b and short-wavelength forms of chl a have been shown to correlate with changes in the intensities of the 726-, 729-, and 731-nm components of the long-wavelength fluorescence. This allows one to assign them to the emission of the outer antenna of Photosystem I. Changes in the intensity of the component at 735 nm correlated only with changes in excitation spectrum in the long-wavelength region that corresponded to the absorption of the long-wave-length forms of chlorophyll a. Therefore, the 735-nm component could be assigned to the emission of the Photosystem I inner antenna. Analysis of the changes induced by heating in the emission and excitation spectra of fluorescence revealed changes in the energy transfer in the outer and the inner antennas of Photosystem I. Heating in the darkness lowered the energy transfer in the outer and in the inner antennas. Both modes of heating in the presence of light increased the energy transfer in the outer antenna. For the inner antenna, presence of the light promotes an efficient of energy transfer at the levels close to the control one. It is proposed that illumination during heating exposure causes a specific state of the antenna complex in Photosystem I that provides an increase in funneling of the energy toward the reaction centers.