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Today the structure of photosystem II, which is the enzyme responsible for the evolution of molecular oxygen by plants, algae and cyanobacteria, is known up to a resolution of about 3.0 Å in cyanobacteria (Loll et al., 2005). Photosystem II of higher plants, which shows some differences compared to the photosystem II of cyanobacteria, is not resolved in such high detail, yet (8-10 Å) (Rhee et al., 1998; Hankamer et al., 2001a). Therefore, the molecular structure of PSII of higher plants and its adjacent antenna complexes remains in the focus of the current research. One of the major problems when working with photosystem II is its relative instability during isolation. Together with the antenna proteins and several other proteins, some of which still have an unclear function, PSII forms a huge multi-protein-complex, which tends to fall apart during classical preparation methods. In order to achieve a faster and milder method of purification for PSII, four different His-tags have been added to one of the subunits of PSII. The gene targeted in this study is called psbE and codes for the α-chain of cytochrome b559, an integral part of PSII. The gene for PsbE is encoded in the chloroplast genome. The His-tags, which were employed in this work, consist of six or ten consecutive histidine aminoacid residues, which were fused to the N-terminus of the protein, either with or without a cleavage site for the protease “Factor Xa”. The N-terminus of PsbE is located on the more accessible stromal side of the thylakoid membrane. After inserting the psbE gene in a vector plasmid, in which the recognition site for the restriction endonuclease SacI had been eliminated, the different His-tags were generated by PCR with purposefully altered primers. In a final cloning step, a gene, which confers resistance to the antibiotics spectinomycin and streptomycin, was added to the DNA construct. Subsequently, the so-called biolistic transformation method (“gene gun”) was applied to introduce this genetically engineered plasmid DNA to Nicotiana tabacum chloroplasts (Bock & Hagemann, 2000). Through the processes of homologous recombination that take place in the chloroplast, the plastid encoded wildtype psbE gene was replaced by its His-tag containing counterparts. After several rounds of regenerating plants on antibiotic-containing medium, successful transformation was confirmed through PCR methods. By self fertilisation of fully regenerated plants, seeds were produced from tobacco strains, which carried only the mutated psbE gene. Plants cultivated from these seeds showed no distinctive phenotype under the chosen growth conditions, in respect to wildtype plants. The presence of the His-tag in this F1 generation was again confirmed with PCR methods. Measurements of oxygen evolution and pulse amplitude modulated fluorescence (PAM), carried out with preparations of wildtype and transgenic tobacco strains, revealed no differences for photochemical or non-photochemical quenching between both types. However, the oxygen evolution capacity of transgenic tobacco thylakoids compared to the wildtype was significantly reduced, although the chlorophyll content in relation to the leaf area was almost identical. This hints at a reduced amount of photosystem II complexes in the thylakoid membranes of transgenic tobacco. This alteration could be related to the mutation of cytochrome b559, because, amongst other functions, this subunit was shown to be important for the assembly of photosystem II (Morais et al., 1998). If solubilised thylakoid preparations of His-tagged plant strains were applied to a Ni-NTA column, photosystem II was selectively bound to the matrix. After washing away most of the contaminations, photosystem II core complexes could be eluted with imidazole-containing buffer. Photosystem II prepared in this way, displayed a drastic reduction of the peripheral light-harvesting complexes (LHCI & LHCII) and photo-system I reaction centres. This could be demonstrated by the loss of chlorophyll b and xanthophyll bands (LHCs) in absorption spectra, a small blue-shift of the chlorophyll a Qy absorption (PSI) and the respective band patterns in polyacrylamide gel electro-phoresis. The photosystem II complexes prepared in this way can now be put to use in different structural studies, like two-dimensional or three-dimensional crystallisation and spectroscopic measurements. Another photosynthetic pigment-protein complex of interest is the fucoxanthin-chlorophyll a/c-binding protein of diatoms, because eukaryotic algae, like diatoms, are important factors of oceanic ecosystems and account for a large part of marine biomass production. In order to facilitate ultra-fast time-resolved transient absorption spectroscopy and subsequent modelling of the kinetic traces, FCPs were prepared by sucrose-gradient ultra-centrifugation and their pigment stoichiometries determined by HPLC. Combining the spectroscopic data (Papagiannakis et al., 2005) with protein sequence alignments (Eppard & Rhiel, 1998) and the structure of the homologous higher plant LHCIIb (Kühlbrandt et al., 1994), a hypothetical model for the structure of FCP could be proposed (Fig. IV.3)
Photosystem (PS) I is a huge membrane protein complex which coordinates around 200 co-factors. Upon light excitation a charge separation at the PS I reaction centre is induced which leads to an electron transport across the thylakoid membrane and the generation of redox equivalents needed for several biochemical reactions, e.g. the synthesis of sugars. For higher plants and cyanobacteria the crystal structure of PS I complexes were resolved to resolutions of 4.4 Å and 2.5 Å. Furthermore, supramolecular structures of PS I of eukaryotic algae, mainly of the green line, were obtained recently. However, up to now, no structure of diatoms is available yet. Diatoms are key players in global primary production and derived from a secondary endosymbiosis event. Their chloroplasts are surrounded by four envelope membranes and their thylakoids are evenly arranged in bands of three, i.e. no separation in grana and stroma regions is apparent. In this thesis a protocol was developed to isolate a functional PS I complex of diatoms which can be used for structural analysis by transmissional electron microscopy (TEM). A photosystem I-fucoxanthin chlorophyll protein (PS I-FCP) complex was isolated from the pennate diatom Phaeodactylum tricornutum by ion exchange chromatography. Spectroscopic analysis proved that bound Fcp polypeptides function as a light-harvesting complex. An active light energy transfer from Fcp associated pigments, Chl c and fucoxanthin, towards the PS I core was proven by fluorescence spectroscopy. Oxidised minus reduced difference spectroscopy evidenced the activity of the PS I reaction centre P700 and yielded a chlorophyll a/P700 ratio of approximately 200:1. These data indicate that the isolated PS I-FCP complex exceeds the PS I cores from cyanobacteria and higher plants in the numbers of chlorophyll a molecules. Because of the strict conservation of PS I cores among organisms the additional 100 chlorophyll a molecules must either be coordinated by Fcps or function as linker molecules between the Fcp antenna and the PS I core as shown for the PS I-LHC I complex of higher plants. To tell something about the structural organisation, the PS I-FCP complex was compared with its cyanobacterial and higher plant counterparts. Whereas cyanobacterial PS I cores aggregate to trimers, usually without associated antennae, higher plant PS I is a monomer and binds additionally two LHC I heterodimers. BN-PAGE and gel filtration experiments showed that also diatoms contain PS I monomers associated with Fcps as light-harvesting antenna. First TEM studies evidenced these observations. Negatively stained PS I-FCP particles had an increased size compared to PS I cores of other organisms. No PS I trimers or higher oligomers have been found. The calculated diameter and shape of the particles correspond to PS I-LHC I particles obtained from green algae, which also comprise of a higher number of LHC I polypeptides compared to the higher plant x-ray structure. Additionally, the analysis of polypeptides indicates that the PS I associated Fcps differ from the free Fcp pool and also from Fcps of a PS II enriched fraction. The assumption that diatoms harbour just one Fcp antenna that serve both Photosystems equally seems to be wrong. To further study the association of Fcps with the two Photosystems, both complexes plus the free FCP complexes were isolated from the centric diatom Cyclotella meneghiniana. Because of the availability of antibodies directed against specific Fcp polypeptides of Cyclotella the PS I-FCP complex of Phaeodactylum could not be used. A trimeric FCP complex, FCPa, and a higher FCP oligomer, FCPb, have already been described for C. meneghiniana. The latter is assumed to be composed of only Fcp5, whereas the FCPa contains Fcp2 and Fcp6. Biochemical and spectroscopical evidences revealed a different subset of associated Fcp polypeptides within the isolated photosystem complexes. Whereas the PS II associated Fcp antenna resembles FCPa, at least three different Fcp polypeptides are associated with PS I. By re-solubilisation of the PS I complex and a further purification step Fcp polypeptides were partially removed from PS I and both fractions were analysed again by biochemical and spectroscopical means, as well as by HPLC. Thereby Fcp4 and a so far undescribed 17 kDa Fcp were found to be strongly coupled to PS I, whereas another Fcp, presumably Fcp5, is only loosely bound to the PS I core. Thus an association of FCPb and PS I is assumed.
The light-harvesting complex of photosystem II (LHC-II) is the major antenna complex in plant photosynthesis. It accounts for roughly 30% of the total protein in plant chloroplasts, which makes it arguably the most abundant membrane protein on Earth, and binds about half of plant chlorophyll (Chl). The complex assembles as a trimer in the thylakoid membrane and binds a total of 54 pigment molecules, including 24 Chl a, 18 Chl b, 6 lutein (Lut), 3 neoxanthin (Neo) and 3 violaxanthin (Vio). LHC-II has five key roles in plant photosynthesis. It: (1) harvests sunlight and transmits excitation energy to the reaction centres of photosystems II and I, (2) regulates the amount of excitation energy reaching each of the two photosystems, (3) has a structural role in the architecture of the photosynthetic supercomplexes, (4) contributes to the tight appression of thylakoid membranes in chloroplast grana, and (5) protects the photosynthetic apparatus from photo damage by non photochemical quenching (NPQ). A major fraction of NPQ is accounted for its energy-dependent component qE. Despite being critical for plant survival and having been studied for decades, the exact details of how excess absorbed light energy is dissipated under qE conditions remain enigmatic. Today it is accepted that qE is regulated by the magnitude of the pH gradient (ΔpH) across the thylakoid membrane. It is also well documented that the drop in pH in the thylakoid lumen during high-light conditions activates the enzyme violaxanthin de-epoxidase (VDE), which converts the carotenoid Vio into zeaxanthin (Zea) as part of the xanthophyll cycle. Additionally, studies with Arabidopsis mutants revealed that the photosystem II subunit PsbS is necessary for qE. How these physiological responses switch LHC-II from the active, energy transmitting to the quenched, energy-dissipating state, in which the solar energy is not transmitted to the photosystems but instead dissipated as heat, remains unclear and is the subject of this thesis. From the results obtained during this doctoral work, five main conclusions can be drawn concerning the mechanism of qE: 1. Substitution of Vio by Zea in LHC-II is not sufficient for efficient dissipation of excess excitation energy. 2. Aggregation quenching of LHC-II does not require Vio, Neo nor a specific Chl pair. 3. With one exception, the pigment structure in LHC-II is rigid. 4. The two X-ray structures of LHC-II show the same energy transmitting state of the complex. 5. Crystalline LHC-II resembles the complex in the thylakoid membrane. Models of the aggregation quenching mechanism in vitro and the qE mechanism in vivo are presented as a corollary of this doctoral work. LHC-II aggregation quenching in vitro is attributed to the formation of energy sinks on the periphery of LHC-II through random interaction with other trimers, free pigments or impurities. A similar but unrelated process is proposed to occur in the thylakoid membrane, by which excess excitation energy is dissipated upon specific interaction between LHC-II and a PsbS monomer carrying Zea. At the end of this thesis, an innovative experimental model for the analysis of all key aspects of qE is proposed in order to finally solve the qE enigma, one of the last unresolved problems in photosynthesis research.
In the present work, the photo-protection mechanisms in plants and purple bacteria were investigated experimentally at the molecular level. For this purpose, several spectroscopic methods were combined and applied to elucidate the function of carotenoids, pigments of the photosynthetic apparatus, in photo-protection. The experiments were focused on the mechanisms involved in quenching of singlet and triplet states of the electronically excited (bacterio)chlorophylls. This photosynthetic reaction events occur on an ultrafast time-scale. Measuring such short-lived events, and understanding the underlying principles, demand some of the most precise experiments and exact measurement technologies currently available. This implies certain requirements for the light source used: a suitable wavelength within the absorption band of the sample, sufficient power, and, most importantly, a pulse duration short compared to the studied reaction. Nowadays, we can achieve all this requirements using femtosecond-spectroscopic systems, which produce laser pulses shorter than 100 femtoseconds (fs). Transient absorption spectroscopy provides important information on molecular dynamics interrogating electronic transitions. The technique is based on photochemical generation of transient species with femtoseconds pump pulses and measuring transient absorption changes of the sample using a second, time delayed probe pulse which in this case is a spectrally broad white-light pulse.
Die bei der Photosynthese verwendete Lichtenergie wird zu einem großen Anteil von Lichtsammlersystemen bereitgestellt. In der pflanzlichen Photosynthese wird unterschieden zwischen Lichtsammlersytem I (light harvesting complex I, LHC-I), assoziiert mit Photosystem I (PS-I) und Lichtsammlersystem II (light harvesting complex II, LHC-II), assoziiert mit Photosystem II (PS-II). LHC-II ist der häufigste Protein-Pigment Komplex der Chloroplasten und bindet bis zu 50% aller Chlorophylle in der Thylakoidmembran. Der Protein-Pigment Komplex LHC-II hat vier, teils miteinander verwandte Funktionen in der Photosynthese. I) Die Sammlung und Weiterleitung von Lichtenergie, II) Stabilisierung der Granastapel, III) Ausgleich der Anregungsenergie von PS-I und PS-II, IV) Schutz der Photosynthese vor Überanregung mittels nichtphotochemischer Eliminierung von Anregungsenergie (NPQ). In der Pflanze bildet LHC-II Trimere in verschiedenen Kombinationen dreier Isoformen (Lhcb1, Lhcb2 und Lhcb3), wobei Lhcb1 mit 70-90% den Hauptteil des LHC-II stellt. Jedes Monomer bindet 8 verschiedene Co-Faktoren in unterschiedlichen Mengen, die ca. 30% seiner Masse ausmachen. Die drei Isoformen des LHC-II sind in allen Pflanzen stark konserviert. Die funktionelle Bedeutung der Isoformen ist jedoch weitestgehend unklar. Dies liegt vor allem an der schwierigen Isolierung reiner Isoformen aus Pflanzenmaterial. Im ersten Teil dieser Arbeit wurden deshalb alle drei Isoformen rekombinant hergestellt und mit getrennt isolierten Lipiden und photosynthetischen Pigmenten in ihre native Form gefaltet. Die anschließende biochemische und spektroskopische Charakterisierung zeigte einen hohen Grad an Homologie zwischen den drei Isoformen, wobei Lhcb3 die größten Unterschiede aufwies (Standfuss und Kühlbrandt 2004). Die wahrscheinlichsten Funktionen für Lhcb1 und Lhcb2 ist die Anpassung der Photosynthese an variierende Lichtbedingungen. LHC-II Heterotrimere mit Lhcb3 Anteil könnten an der Weiterleitung von Lichtenergie von der Haupt Lhcb1/Lhcb2 Antenne zum PS-II Reaktionszentrum beteiligt sein. Für die Erforschung des LHC-II war das mittels Cryo-Elektronenmikroskopie an 2D Kristallen erstellte atomare Modell des Komplexes von enormer Bedeutung. Ein tiefes Verständnis der Funktionen des LHC-II benötigt jedoch eine Struktur von höherer Auflösung, welche mit 2D Kristallen nur schwer zu erreichen ist. Im Verlauf der Arbeit wurden deshalb mehr als 100000 3D Kristallisationsexperimente durchgeführt, wodurch die Kristallisation von aus Erbsenblättern isoliertem und in vitro gefaltetem LHC-II gelang. Die 3D Kristalle aus nativem Material zeigten einen für die röntgenkristallographische Strukturaufklärung ausreichenden Ordnungsgrad und führten zu einer Struktur des LHC-II bei 2.5 Å Auflösung (Standfuss et al., eingereicht). Die Struktur zeigt 223 der 232 Aminosäuren und die Position und Orientierung von 4 Carotinoiden (2 Luteine, 1 Neoxanthin und 1 Violaxanthin), 14 Chlorophyllen (8 Chl a und 6 Chl b) und zwei Lipiden (PG und DGDG) pro Monomer. Diese Informationen sind essentiell für das Verständnis des Energietransfers innerhalb des LHC-II und zu den Photoreaktionszentren und sollten zusammen mit der großen Anzahl von spektroskopischen Untersuchungen eine zukünftige detaillierte Modellierung dieser ultraschnellen und extrem effizienten Energietransfer Prozesse ermöglichen. Auf Basis der Ladungsverteilung der stromalen Seite des Komplexes konnte ein Modell für die Beteiligung des LHC-II an der Stapelung von Grana in Chloroplasten erstellt werden. Dieses liefert außerdem eine plausible Erklärung für den mittels Phosphorylierung des N-Terminus gesteuerten Ausgleich von Anregungsenergie zwischen PS-I und PS-II. Die 2.5 Å Struktur des LHC-II zeigt schließlich einen einfachen aber effektiven Mechanismus zur Optimierung und Schutz des Photosyntheseapparates mittels NPQ. Dieser benötigt keine Strukturänderungen des LHC-II oder der restlichen Lichtsammelantenne und beruht auf der reversiblen Bindung der Xanthophylle Violaxanthin und Zeaxanthin an LHC-II. Diese Arbeit liefert damit Beiträge zu allen Funktionen des LHC-II Komplexes und hilft damit grundlegende Regulationsmechanismen und die Bereitstellung von solarer Energie für die pflanzliche Photosynthese zu verstehen.
Time-resolved spectroscopic analysis of fucoxanthin-chlorophyll proteins and isolated carotenoids
(2011)
The aim of this thesis was to elucidate the excitation energy transfer in the fucoxanthin-chlorophyll proteins (FCPs) isolated from the diatom Cyclotella meneghiniana in detail and to clarify the role of the different pigments contained. In a first step the excited state dynamics of the free pigments were studied by means of time-resolved absorption spectroscopy. The FCPs contain three different carotenoid species. Besides the main light-harvesting carotenoid fucoxanthin (fx) the xanthophyll cycle pigments diadinoxanthin (ddx) and diatoxanthin (dtx) are found in substoichiometric amounts. Fx is contained in an unusual carotenoid-to-chlorophyll ratio of about one. In case of ddx and dtx, changing the solvent polarity showed no significant effects on the absorption spectrum and the excited state dynamics were hardly influenced. In contrast, a solvent dependence is observed in the absorption spectrum and excited state dynamics of fx. The S1 lifetime depends strongly on the solvent polarity and an additional broad excited state absorption band red shifted compared to the S1 excited state absorption appears. The occurrence of the described features can be explained with an intramolecular charge transfer state, which is stabilized in a polar environment and appears only in carotenoids with a conjugated carbonyl group. Despite its rather short excited state lifetimes of less than 200 fs (S2) and 30-60 ps (S1), fx acts as a very efficient energy donor in the FCPs. The ultrafast energy transfer dynamics of the isolated proteins FCPa and FCPb were investigated in a comprehensive study using transient absorption in the visible and NIR spectral region complemented with polarized transient absorption spectroscopy. The excitation energy transfer was not influenced significantly by changing the light conditions during the growth, which yields an altered amount of ddx and dtx. It can be concluded that the contribution of the xanthophyll cycle pigments to the energy transfer is not significant. The altered oligomerization state results in a more efficient energy transfer for the trimeric FCPa, which is also reflected in different Chl a fluorescence quantum yields. Thus, an increased quenching in the higher oligomers of FCPb can be assumed. The observed dynamics change drastically for two different excitation wavelengths λ = 500 nm and λ = 550 nm, which both lead to the population of the S2 excited state of individual carotenoids, namely blue and red absorbing fx molecules. The differing absorption maxima result from distinct microenvironments within the protein. For FCPa an additional slow time constant of 25 ps was found after excitation at 500 nm. By means of polarized transient absorption spectroscopy applied to FCPa different transition dipole moments for the S1 and the ICT state of fx could be identified. Based on the presented studies a detailed model explaining the excitation energy transfer pathways could be developed. In agreement with the faster overall transfer rate which is also evident in the anisotropy data in case of 550 nm excitation, upon excitation at 500 nm one slow transfer channel is active. It can be attributed to a blue absorbing fx not strongly associated with a Chl a molecule. Most likely excitation energy transfer takes place between the S1/ICT states of two different fx molecules before the energy is transferred to Chl a. Additional transient absorption experiments with an improved time resolution were performed to investigate the oscillations observed. These coherent effects superimposed the kinetics of isolated carotenoids as well as FCPs within the first 500 fs. The oscillations showed a very unusual damping behavior and vanished already after two oscillation periods. In case of fx, the solvent environment as well as the excitation wavelengths had an influence on the oscillations. The frequencies of the oscillations were 70-100 cm^-1 for fx in solvents with varying polarity and 50-80 cm^-1 for the FCPs. These results could further confirm the assumption that the red absorbing fx molecules are located in a more polar environment within the protein compared to the blue absorbing fx. To clarify the origin of the oscillations in more detail, further experiments with a controlled chirp of the applied pulses and comparison between different carotenoids in various solvents are required. This approach promises to give further insight in the excited state dynamics and to answer the question whether dark states are involved. Right now, the coherent excitation of the strongly coupled excited states 1Bu+ (S2) and 1Bu- resulting in electronic quantum beats and the existence of an additional short lived excited state absorption (S2-SN2) in the visible spectral region are the most reasonable explanations for the occurrence of the coherent effects in the transient absorption spectra of carotenoids.