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The six-membered ring of the title compound, C11H16NO, has a distorted envelope conformation. The piperidine N atom deviates by 0.128 (1) Å from the plane through its three neighbouring atoms. In the crystal structure, molecules are connected by intermolecular Cethynyl-H...O contacts to form chains extending in the [10\overline{1}] direction. Key indicators: single-crystal X-ray study; T = 167 K; mean σ(C–C) = 0.001 Å ; R factor = 0.040; wR factor = 0.112; data-to-parameter ratio = 27.3.
The five-membered ring of the title compound, C10H14NO, is almost planar [mean deviation from best plane = 0.006 (1) Å]. The N-O bond is in the plane of the five-membered ring. The molecule is positioned about a pseudo-mirror plane at y = 0.375. In the crystal, molecules are connected by intermolecular C-H...O contacts into layers parallel to (010). Key indicators: single-crystal X-ray study; T = 167 K; mean σ(C–C) = 0.002 Å; R factor = 0.062; wR factor = 0.157; data-to-parameter ratio = 27.3.
Na+/H+ antiporters are ubiquitous membrane proteins involved in ion homeostasis and pH sensing. The amino acid sequence of one such antiporter, MjNhaP1, from Methanococcus jannaschii, shows a significant homology to eukaryotic sodium proton exchangers like NHE1 from Homo sapiens and SOS1 of Arabidopsis thaliana than to the well-characterized Escherichia coli NhaA or NhaB. MjNhaP1 shows activity at acidic pH unlike NhaA, which is active at basic pH. 13 transmembrane helices have been predicted to be present in NhaP1. A projection map, calculated by Cryo-EM of 2D crystals of MjNhaP1 grown at pH 4, showed it to be a dimer containing elongated densities in the centre of the dimer and a cluster of density peaks on either side of the dimer core (Vinothkumar et al., 2005). Incubation of 2D crystals at pH 8 on the EM grid resulted in well-defined conformational changes, clearly evident in a difference map as a major change in density distribution within the helix bundle (Vinothkumar et al., 2005). The aim of this dissertation is to understand the working mechanism of MjNhaP1 by determining its three-dimensional structure. The aim was initially approached by structure determination by X-ray crystallography. The limitation for this method was the low expression yield, which was 0.5–0.7mg/ml (Vinothkumar et al., 2005). After various optimization trials, the expression yield of the recombinant protein could be elevated to 2-2.5mg of pure protein per litre of culture by the method of autoinduction (Studier et al., 2005). To obtain well diffracting 3D crystals, purification conditions (Vinothkumar et al., 2005) were modified. 3D crystals were obtained under various conditions, which has so far not diffracted X-Ray beyond 8Å. Parallely, optimization of parameters (Vinothkumar et al., 2005) for 2D crystals formation was carried out. A combination of 1% DDM used for lipid solubilization, and 1% OG in the buffer of the purified protein produced 1-2 μm wide tubular 2D crystals of NhaP1. This batch of crystal proved to be the optimal for data collection at higher tilt angle with the electron microscope. A 3D map showed p22121 symmetry and revealed a tight dimer with an oval shape. The region in the central part of the dimer is composed of several tilted helices forming an interface between both monomers. On either side of the dimer interface, a group of six tightly packed helices form a bundle. This bundle contains three straight helices in the centre of the monomer and three helices in the periphery. Comparison of the structures of E.coli NhaA and M. jannaschii NhaP1 show substantial differences in length and slope of corresponding helices between both antiporters. A 3D model of NhaP1 based on the 3D map revealed 13 helices, which has been named as A-M to distinguish it from the NhaA helices. Overlaying the X-ray structure onto the 3D map revealed that the disrupted helices IV and XI of NhaA superimpose two central helices at similar position in the 3D map of NhaP1. The disrupted helices IV and XI in the X-ray structure of NhaA have been proposed as the putative ion-binding and translocation site (Hunte C et al, 2005; Arkin IT et al, 2007; Screpanti & Hunte (2007). This motif appears to be present also in NhaP1, as suggested by the close fit of NhaA helices IV and XI on the putative helices E and L of the NhaP1 model. These two putative helices E and L in NhaP1 contain the highly conserved TDP and GPRVVP motif, which are crucial for antiporter activity (Hellmer et al., 2002, Hellmer et al., 2003). In the overlay, helix V of NhaA containing the two essential, conserved aspartates D163 and D164 fits the density of the putative helix F of NhaP1, which contains the conserved motif FNDP. The homologous D161 in the FNDP motif of NhaP1 is essential for transport activity as show by mutagenesis (Hellmer at al., 2003). Significant differences are visible in the region of the dimer interface of the 3D map of NhaP1 occupied by helices VI, VII, and VIII in NhaA. This region shows an extra helical density (A) in the 3D map of NhaP1. By alignment of MjNhaP1 sequence with the amino acid sequences of several Na+/H+ exchangers, it was evident that the additional helix (A) is located in the N terminus of NhaP1. In our sequence alignment, a putative hydrophobic segment corresponding to this additional helix A is present in other archaeal and eukaryotic antiporters but not in any of the bacterial ones. The N-terminus of the human Na+/H+ exchanger NHE1 has been predicted to contain a highly hydrophobic signal peptide. This indicates the probability of the N-terminal helix A of NhaP1 to be an uncleaved signal peptide. Besides being a signal sequence targeting NhaP1 to the membrane, the map suggests that this helix might be involved in the formation of dimer contacts between both monomers. A gene duplication event is evident in the 3D map of NhaP1, as not only the helices D, E, F and K, L, M are related by an inverted repeat but also the helices B, C and I, J are related. We present here the three-dimensional architecture of a Na+/H+ antiporter from archaea. The presence of the 13th helix suggests the location of the N-terminus to be located in the cytosol and the C-terminus in the periplasm. This would orient NhaP1 in an inverted manner in the membrane in comparison to NhaA. Further structural information at higher resolution and biochemical and biophysical investigations are required to confirm the topology.
1. Fab co-complexes of proton pumping NADH:ubiquinone oxidoreductase (complex I) Fab fragments suitable for co-crystallization with complex I were generated using an immobilized papainbased protocol. The binding of the antibody fragments to complex I was verified using Surface Plasmon Resonance and size exclusion chromatography. The binding constants of the antibodies and their respective Fab fragments were found to be in the nanomolar range. This work presents the first report on successful crystallization of complex I (proton pumping NADH:ubiquinone oxidoreductase) from Yarrowia lipolytica with proteolytic Fab fragments. The quality of the crystals was significantly improved when compared to the initial experiments and the best crystals diffracted X-rays to a resolution of ~7 Å. The activity of complex I remained uninfluenced by antibody fragment binding. The initial diffraction data suggest that the complex I/Fab co-complex crystals represent a space group different to the one observed for the native protein. Ongoing experiments are aimed at further enhancements of the diffraction quality of the crystals. Providing a different space group the CI/Fab co-complexes may become a very useful approach for structure determination of the enzyme. Moreover, the bound Fab offers an additional possibility to generate phase information. The antibody-mediated crystallization represents a valuable tool in structural characterization of the NADH:oxidoreductase subcomplexes or even single subunits. 2. UDP-glucose pyrophosphorylase UDP-glucose pyrophosphorylase from Yarrowia lipolytica displays affinity towards Ni2+ NTA and was first detected in a contaminated sample of complex I. Following, separation from complex I, Ugp1p was purified using anion exchange chromatography. Sequence similarity studies revealed high identity to other known pyrophosphorylases. As indicated by laser-based mass spectrometry method (LILBID) Ugp1p from Y. lipolytica builds octamers similarly to the enzyme from Saccharomyces cerevisiae. The initial crystals grew as thin needles favorably in sitting drop setups. The size of the crystals was increased by employment of a micro batch technique. The improved crystals diffracted X-rays to a resolution of 3.2 Å at the synchrotron beamline. Structural characterization is under way using a molecular replacement approach based on the published structure of baker’s yeast UGPase.
P2X receptors represent the third superfamily of ligand gated ion channels with ATP as their natural ligand. Most of the mammalian P2X receptors are non-selective cation channels, which upon activation, mediate membrane depolarization and have physiological roles ranging from fast excitatory synaptic transmission, modulation of pain-sensation, LTP to apoptosis etc. In spite of them being an attractive drug target, their potential as a drug target is limited by the lack of basic understanding of the structure-function relationship of these receptors. In my thesis, I have investigated the behavior of homomeric P2X receptor subunits with the help of photolabeling and fluorescence techniques coupled to electrophysiological measurements using Xenopus laevis oocytes heterologous expression system. Concurrent photolabeling by BzATP and current recordings from the same set of receptors in real time has revealed that the gating process in homomeric P2X receptors is contributed individually by each subunit in an additive manner. Our study for the first time describes the agonist potency of Alexa-ATP (a fluorescent ATP analog) on P2X1 receptors. The use of Alexa-ATP in our experiments elucidated that receptor subunits are not independent but interacting with each other in a cooperative manner. The type of cooperativity, however, depended on the type and concentrations of allosteric/competing ligands. Based on our results, in my thesis we propose an allosteric model for ligand-receptor interactions in P2X receptors. When simulated, the model could replicate our experimental findings thus, further validating our model. Further, correlation between occupancy of P2X1 receptors (determined using binding curve for Alexa-ATP) with the steady-state desensitization suggests that binding of three agonist molecules per receptor are required to desensitize P2X1 receptors. We further extended the approach of fluorescence with electrophysiological measurement to assign the role for different domains in P2X1 receptors with the help of environmental sensitive, cysteine reactive fluorophore (TMRM). Cysteine rich domain-1 of P2X1 receptors (C117-C165) was found to be involved in structural rearrangements after agonist and antagonist binding. In contrast to the present understanding, that the binding of an antagonist cannot induce desensitization in P2X1 receptors and the receptors need to open first before undergoing desensitization, we propose based on our results that a competitive antagonist can also induce desensitization in P2X1 receptors by bypassing the open state. We have attempted to answer few intriguing questions in the field of P2X receptor research and we think that our answers provide many avenues to the basic understanding of functioning of P2X receptors.
Lentiviral vectors mediate gene transfer into dividing and most non-dividing cells. Thereby, they stably integrate the transgene into the host cell genome. For this reason, lentiviral vectors are a promising tool for gene therapy. However, safety and efficiency of lentiviral mediated gene transfer still needs to be optimised. Ideally, cell entry should be restricted to the cell population relevant for a particular therapeutic application. Furthermore, lentiviral vectors able to transduce quiescent lymphocytes are desirable. Although many approaches were followed to engineer retroviral envelope proteins, an effective and universally applicable system for retargeting of lentiviral cell entry is still not available. Just before the experimental work of this thesis was started, retargeting of measles virus (MV) cell entry was achieved. This virus has two types of envelope glycoproteins, the hemagglutinin (H) protein responsible for receptor recognition and the fusion (F) protein mediating membrane fusion. For retargeting, the H protein was mutated in its interaction sites for the native MV receptors and a ligand or a single-chain antibody (scAb) was fused to its ectodomain. It was hypothesised that the retargeting system of MV can be transferred to lentiviral vectors by pseudotyping human immunodeficiency virus-1 (HIV-1) derived vector particles with the MV glycoproteins. As the unmodified MV glycoproteins did not pseudotype HIV vectors, two F and 15 H protein variants carrying stepwise truncations or amino acid (aa) exchanges in their cytoplasmic tails were screened for their ability to form MV-HIV pseudotypes. The combinations Hcd18/Fcd30, Hcd19/Fcd30 and Hcd24+4A/Fcd30 led to most efficient pseudotype formation with titers above 10exp6 transducing units /ml, using concentrated particles. The F cytoplasmic tail was truncated by 30 aa and the H cytoplasmic tail was truncated by 18, 19 or 24 residues with four added alanines after the start methionine in the latter case. Western blot analysis indicated that particle incorporation of the MV glycoproteins was enhanced upon truncation of their cytoplasmic tails. With the MV-HIV vectors high titers on different cell lines expressing one or both MV receptors were obtained, whereas MV receptor-negative cells remained untransduced. Titers were enhanced using an optimal H to F plasmid ratio (1:7) during vector particle production. Based on the described pseudotyping with the MV glycoprotein variants, HIV vectors retargeted to the epidermal growth factor receptor (EGFR) or the B cell surface marker CD20 were generated. For the production of the retargeted vectors MVaEGFR-HIV and MVaCD20-HIV, Fcd30 together with a native receptor blind Hcd18 protein, displaying at its ectodomain either the ligand EGF or a scAb directed against CD20 were used. With these vectors, gene transfer into target receptor-positive cells was several orders of magnitude more efficient than into control cells. The almost complete absence of background transduction of non-target cells was e.g. demonstrated in mixed cell populations, where the CD20-targeting vector selectively eliminated CD20-positive cells upon suicide gene transfer. Remarkably, transduction of activated primary human CD20-positive B cells was much more efficient with the MVaCD20-HIV vector than with the standard pseudotype vector VSV-G-HIV. Even more surprisingly, MVaCD20-HIV vectors were able to transduce quiescent primary human B cells, which until then had been resistant towards lentiviral gene transfer. The most critical step during the production of MV-HIV pseudotypes was the identification of H cytoplasmic tail mutants that allowed pseudotyping while retaining the fusion helper function. In contrast to previously inefficient targeting strategies, the reason for the success of this novel targeting system must be based on the separation of the receptor recognition and fusion functions onto two different proteins. Furthermore, with the CD20-targeting vector transduction of quiescent B cells was demonstrated for the first time. Own data and literature data suggest that CD20 binding and hyper-cross-linking by the vector particles results in calcium influx and thus activation of quiescent B cells. Alternatively this feature may be based on a residual binding activity of the MV glycoproteins to the native MV receptors that is insufficient for entry but induces cytoskeleton rearrangements dissolving the post-entry block of HIV vectors. Hence, in this thesis efficient retargeting of lentiviral vectors and transduction of quiescent cells was combined. This novel targeting strategy should be easily adaptable to many other target molecules by extending the modified MV H protein with appropriate specific domains or scAbs. It should now be possible to tailor lentiviral vectors for highly selective gene transfer into any desired target cell population with an unprecedented degree of efficiency.
Large amplitude intramolecular motions in non-rigid molecules are a fundamental issue in chemistry and biology. The conventional approaches for study these motions by far-infrared and microwave spectroscopy are not applicable when the molecule is non-polar. Therefore, in the current thesis an alternative approach for the investigation of large amplitude intramolecular motions was developed and tested. This new method is based on femtosecond rotational degenerate four-wave mixing spectroscopy (fs DFWM), which is a particular implementation of rotational coherence spectroscopy. The method was successfully applied for the investigation of pseudorotation in pyrrolidine and the ring-puckering vibration in cyclopentene. Another important subject is the photophysics of molecules and molecular clusters which have an ultrashort lifetime of their electronically excited state (photoreactivity). These ultrashort lifetimes often represent a protective mechanism causing photostability. The photoreactivity is usually the manifestation either of an “elementary” reaction, such as proton or electron transfer, which occurs in the excited state or of a fast non-radiative deactivation processes, such as internal conversion via conical intersection of the electronically excited and ground state. Due to a short-lived excited state, the conventional vibrational spectroscopic methods, such as IR depletion detected by resonance two-photon ionization spectroscopy (IR/R2PI), are not applicable for the structural investigation of these systems. Therefore, new approach, termed IR depletion detected by multiphoton ionization with femtosecond laser pulses (IR/fsMPI), was developed for studying the structure of photoreactive microsolvated molecules. The IR/fsMPI technique was applied for investigating the clusters of 1H-pyrrolo[3,2-h]quinoline with water/methanol as well as adenine- and 9-methyl-adenine-hydrates. In addition, the excited state dynamics of bifunctional azaaromatic molecule 7-(2'-pyridyl)indole (7PyIn) was studied by femtosecond pump-probe resonance excitation multiphoton ionization technique (fs REMPI). Under electronic excitation of this molecule a fast proton transfer (phototautomerization) takes place, which is followed by radiationless excited state deactivation process. The fs REMPI spectra lead to the conclusion that the phototautomerization in 7PyIn is coupled with a twisting of the molecule, and that the twisting provides an efficient channel for ultrafast radiationless excited state deactivation. This pattern of excited-state tautomerization/deactivation might be quite general.
By adopting a variety of shapes, proteins can perform a wide number of functions in the cell, from being structural elements or enabling communication with the environment to performing complex enzymatic reactions needed to sustain metabolism. The number of proteins in the cell is limited by the number of genes encoding them. However, several mechanisms exist to increase the overall number of protein functions. One of them are post-translational modifications, i.e. covalent attachment of various molecules onto proteins. Ubiquitin was the first protein to be found to modify other proteins, and, faithful to its evocative name, it is involved in nearly all the activities of a cell. Ubiquitylation of proteins was believed for a long time only to be responsible for proteasomal degradation of modified proteins. However, with the discovery of various types of ubiquitylation, such as mono-, multiple- or poly-ubiquitylation, new functions of this post-translational modification emerged. Mono-ubiquitylation has been implicated in endocytosis, chromatin remodelling and DNA repair, while poly-ubiquitylation influences the half-life of proteins or modulates signal transduction pathways. DNA damage repair and tolerance are example of pathways extensively regulated by ubiquitylation. PCNA, a protein involved in nearly all types of DNA transaction, can undergo both mono- and poly-ubiquitylation. These modifications are believed to change the spectrum of proteins that interact with PCNA. Monoubiquitylation of PCNA is induced by stalling of replication forks when replicative polymerases (pols) encounter an obstacle, such as DNA damage or tight DNA-protein complexes. It is believed that monoubiquitylation of PCNA stimulates the exchange between replicative pols to one of polymerases that can synthesize DNA across various lesions, a mechanism of damage tolerance known as translesion synthesis (TLS). Our work has helped to understand why monoubiqutylation of PCNA favours this polymerase switch. We have identified two novel domains with the ability to bind Ub non-covalently. These domains are present in all the members of Y polymerases performing TLS, and were named Ub-binding zinc finger (UBZ) (in polη and polκ) and Ub-binding motif (UBM) (in polι and Rev1). We have shown that these domains enable Y polymerases to preferentially gain access to PCNA upon stalling of replication, when the action of translesion polymerases is required. While the region of direct interaction between Y pols and PCNA had been known (BRCT domain in Rev1 and PIP box motif (PIP) in three others members), we propose that Ub-binding domains (UBDs) in translesion Y pols enhance the PIP- or BRCT-domain-mediated interaction between these polymerases and PCNA by binding to the Ub moiety attached onto PCNA. Following these initial studies, we have also discovered that Y polymerases themselves undergo monoubiquitylation and that their UBDs mediate this modification. This auto-ubiquitylation is believed to lead to an intramolecular interaction between UBD and Ub attached in cis onto the UBD-containing protein. We have mapped monoubiquitylation sites in polη in the C-terminal portion of the protein containing the nuclear localization signal (NLS) and the PIP box. Beside PIP, the NLS motif is also involved in direct interaction of polη with PCNA. Based on these findings, we propose that monoubiquitylation of either NLS or PIP masks them from potential interaction with PCNA. Lastly, using several functional assays, we have demonstrated the importance of all these three motifs in the C-terminus of polη (UBZ, NLS and PIP) for efficient TLS. We have also constructed a mimic of monoubiquitylated polη by genetically fusing polη with Ub. Interestingly, this chimera is deficient in TLS as compared to the wild-type protein. Altogether, these studies demonstrate that the C-terminus of polη constitutes a regulatory module involved in multiple-site interaction with monoubiquitylated PCNA, and that monoubiquitylation of this region inhibits the interaction between polη and PCNA. Our work has also revealed that the UBDs of Y pols as well as of other proteins implicated in DNA damage repair and tolerance, such as the Werner helicase-interacting protein 1 (Wrnip1), are required for their proper sub-nuclear localization. All these proteins localize to discrete focal structures inside the nucleus and mutation of their UBDs results in inability to accumulate in these foci. Interestingly, by exchanging UBDs between different proteins we have learned that each UBD seems to have a distinct functional role, surprisingly not limited to Ubbinding ability. In fact, swapping the UBZ of Wrnip1 with the UBM of polι abolished the localization of Wrnip1 to foci despite preserving the Ub-binding ability of the chimeric protein. In summary, this work provides an overview of how post-translation modification of proteins by Ub can regulate several DNA transactions. Firstly, key regulators (e.g. PCNA) can be differentially modified by Ub. Secondly, specialized UBDs (e.g. UBM, UBZ) embedded only in a subset of proteins act as modules able to recognize these modifications. Thirdly, by means of mediating auto-ubiquitylation, UBDs can modulate the behaviour of host proteins by allowing for either in cis or in trans Ub-UBD interactions.
High-resolution NMR structure of an RNA model system : the 14-mer cUUCGg tetraloop hairpin RNA
(2009)
We present a high-resolution nuclear magnetic resonance (NMR) solution structure of a 14-mer RNA hairpin capped by cUUCGg tetraloop. This short and very stable RNA presents an important model system for the study of RNA structure and dynamics using NMR spectroscopy, molecular dynamics (MD) simulations and RNA force-field development. The extraordinary high precision of the structure (root mean square deviation of 0.3 Å) could be achieved by measuring and incorporating all currently accessible NMR parameters, including distances derived from nuclear Overhauser effect (NOE) intensities, torsion-angle dependent homonuclear and heteronuclear scalar coupling constants, projection-angle-dependent cross-correlated relaxation rates and residual dipolar couplings. The structure calculations were performed with the program CNS using the ARIA setup and protocols. The structure quality was further improved by a final refinement in explicit water using OPLS force field parameters for non-bonded interactions and charges. In addition, the 2'-hydroxyl groups have been assigned and their conformation has been analyzed based on NOE contacts. The structure currently defines a benchmark for the precision and accuracy amenable to RNA structure determination by NMR spectroscopy. Here, we discuss the impact of various NMR restraints on structure quality and discuss in detail the dynamics of this system as previously determined.
Photo-initiated processes, like photo-excitation and -deexcitation, internal conversion, excitation energy transfer and electron transfer, are of importance in many areas of physics, chemistry and biology. For the understanding of such processes, detailed knowledge of excitation energies, potential energy surfaces and excited state properties of the involved molecules is an essential prerequisite. To obtain these informations, quantum chemical calculations are required. Several quantum chemical methods exist which allow for the calculation of excited states. Most of these methods are computationally costly what makes them only applicable to small molecules. However, many biological systems where photo-processes are of interest like light-harvesting complexes in photosynthesis or the reception of light in the human eye by rhodopsin are quite large. For large systems, however, only few theoretical methods remain applicable. The currently most widely used method is time-dependent density functional theory (TD-DFT), which can treat systems of up to 200–300 atoms with the excitation energies of some excited states exhibiting errors of less than 0.5 eV. Yet, TD-DFT has several drawbacks. The most severe failure of TD-DFT is the false description of charge transfer states which is particularly problematic in case of larger systems where it yields a multitude of artificially low-lying charge transfer states. But also Rydberg states and states with large double excitation character are not described correctly. Still, if these deficiencies are kept in mind during the interpretation of results, TD-DFT is a useful tool for the calculation of excited states. In my thesis, TD-DFT is applied in investigations of excitation energy and electron transfer processes in light-harvesting complexes. Since light-harvesting complexes, which consist of thousands of atoms, are by far too large to be calculated, model complexes for the processes of interest are constructed from available crystal structures. The model complexes are used to calculate potential energy curves along meaningful reaction coordinates. Artificial charge transfer states are corrected with the help of the so-called ∆DFT method. The resulting potential energy curves are then interpreted by comparison with experimental results. For the light-harvesting complex LH2 from purple bacteria the experimentally observed formation of carotenoid radical cations is studied. It is shown that the carotenoid radical cation is formed most likely via the optically forbidden S1 state of the carotenoid. In light-harvesting complex LHC-II of green plants the fast component of the so-called non-photochemical quenching (NPQ) is investigated. Two of several different hypotheses on the mechanism of NPQ, which have been proposed recently, are studied in detail. The first one suggests that NPQ proceeds via simple replacement of violaxanthin by zeaxanthin in the binding pocket in LHC-II. However, the calculated potential energy curves exhibit no difference between violaxanthin and zeaxanthin in the binding pocket. In combination with experimental results it is thus shown that simple replacement alone does not mediate NPQ in LHC-II. The second hypothesis proposes conformational changes of LHC-II that lead to quenching at the central lutein and chlorophyll molecules during NPQ. My TD-DFT calculations demonstrate that if this mechanism is operative, only the lutein 1 which is one of two central luteins present in LHC-II can take part in the quenching process. This is corroborated by recent experiments. Though several conclusions can be drawn from the investigations using TD-DFT, the interpretability of the results is limited due to the deficiencies of the method and of the models. To overcome the methodological deficiencies, more accurate methods have to be employed. Therefore, the so-called algebraic diagrammatic construction scheme (ADC) is implemented. ADC is a widely overlooked ab initio method for the calculation of excited states, which is based on propagator theory. Its theoretical derivation proceeds via perturbation expansion of the polarization propagator, which describes electronic excitations. This yields separate schemes for every order of perturbation theory. The second order scheme ADC(2), which is employed here, is the equivalent to the Møller-Plesset ground state method MP(2), but for excited states. It represents the computationally cheapest excited state method which can correctly describe doubly excited states, as well as Rydberg and charge transfer states. The quality of ADC(2) results is demonstrated in calculations on linear polyenes which serve as model systems for the larger carotenoid molecules. The calculations show that ADC(2) describes the three lowest excited states of polyenes sufficiently well, particularly the optically forbidden S1 state which is known to possess large double excitation character. Yet, the applicability of the method is limited compared to TD-DFT due to the much larger computational requirements. To facilitate the calculation of larger systems with ADC(2) a new variant of the method is developed and implemented. The variant employs the short-range behavior of electron correlation to reduce the computational effort. As a first step, the working equations of ADC(2) are transformed into a basis of local orbitals. In this basis negligible contributions of the equations which are due to electron correlation can be identified based on the distances of local orbitals. A so-called “bumping” scheme is implemented which removes the negligible parts during a calculation. This way, the computation times as well as the disk space requirements can be reduced. With the “bumping” scheme several new parameters are introduced that regulate the amount of “bumping” and thereby the speed and the accuracy of computations. To determine useful values for the parameters an evaluation is performed using the linear polyene octatetraene as test molecule. From the evaluation an optimal set of parameter values is obtained, so that the computation times become minimal, while the errors in the excitation energies due to the “bumping” do not exceed 0.15 eV. With further calculations on various molecules of different sizes it is tested if these parameter values are universal, i.e. if they can be used for all molecules. The test calculations show that the errors in the excitation energies are below 0.15 eV for all test systems. Additionally, no trend is visible for the errors that their magnitude might depend on the system. In contrast, the amount of disregarded contributions in the calculations increases drastically with growing system size. Thus, the local variant of ADC(2) can be used in future to reliably calculate excited states of systems which are not accessible with conventional ADC(2).