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GPCRs and ligand-gated ion channels mediate a great variety of physiological effects within the human brain and periphery. The search for selective ligands at these target sites as pharmacological tools or new drug candidates is of great interest. With increasing knowledge of the great diversity of some receptor families, compounds formerly considered to be selective, turned out to be non-selective with regard to recently identified subtypes, splice variants or additional receptor subunits. This work provides SAR studies by means of radioligand binding experiments at serotonergic h5-HT3A and h5-HT4(b) receptors, histamine hH1 receptors and muscarinic hM1-5 receptors. ...
Resistive Plate Chambers (RPCs) are gaseous parallel plate avalanche detectors that implement electrodes made from a material with a high volume resistivity between 10 high 7 and 10 high 12 omega cm. Large area RPCs with 2mm single gaps operated in avalanche mode provide above 98% efficiency and a time resolution of around 1 ns up to a flux of several kHz/cm high 2. These Trigger RPCs will, as an example, equip the muon detector system of the ATLAS experiment at CERN on an area of 3650 m high 2 and with 355.000 independent read out channels. Timing RPCs with a gas gap of 0.2 to 0.3mm are widely used in multi gap configurations and provide 99% efficiency and time resolution down to 50 ps. While their performance is comparable to existing scintillator-based Time-Of-Flight (TOF) technology, Timing RPCs feature a significantly, up to an order of magnitude, lower price per channel. They will for example equip the 176 m high 2 TOF barrel of the ALICE experiment at CERN with 160.000 independent read out cells. RPCs were originally operated in streamer mode providing large signals which simplifies readout electronics and gap uniformity requirements. However, high rate applications and detector aging issues made the operation in avalanche mode popular. This was also facilitated by the development of new highly quenching C2F4H2-based gas mixtures with small contents of SF6. While the physics of streamers is difficult to study, the avalanche mode opened the possibility for a detailed simulation of the detector physics processes in RPCs. Even though RPCs were introduced in the early eighties and have been (will be) used in experiments, there are still disagreements about the explanation of several aspects of the RPC performance. The high efficiency of single gap RPCs would require a large ionization density of the used gases, which according to some authors contradicts measurements. Even in the case of a large ionization density the gas gain has to be extremely large, in order to arrive at the observed RPC efficiency. This raises other questions: A very strong space charge effect is required to explain the observed small avalanche charges around 1 pC. Doubts have been raised whether an avalanche can progress under such extreme conditions without developing into a streamer. To overcome these difficulties, other processes, like the emission of an electron from the cathode, were suggested. Moreover, the shape of measured charge spectra of single gap RPCs differs largely from what is expected from the statistics of the primary ionization and the avalanche multiplication. In this thesis we discuss the detector physics processes of RPCs, from the primary ionization and the avalanche statistics to the signal induction and the read out electronics. We present Monte-Carlo simulation procedures that implement the described processes. While the fundament of the described model and some results were already published elsewhere [1], the subject of this thesis is the implementation of the space charge effect. We present analytic formulas for the electrostatic potential of a point charge in the gas gap of an RPC. These formulas were developed in collaboration with the University of Graz [2] and were published in [3, 4]. The simulation model presented in [1] is completed by the dynamic calculation of the space charge field using these formulas. Since the gas parameters like drift velocity and the Townsend and attachment coefficients depend on the electric field, they are calculated dynamically as well. The functional dependence of these parameters on the field is obtained with the simulation programs MAGBOLTZ and IMONTE. For the primary ionization parameters, we use the values that are predicted by the program HEED. While the described procedure only simulates the longitudinal avalanche development towards the anode of the RPC, we also present more dimensional models that allow a careful study of the transverse repulsive and attractive forces of the space charge fields, and of the consequences for the avalanche propagation. We shall show that the efficiencies of single gap Timing RPCs is indeed explained by the high primary ionization density (about 9.5 /cm as predicted by HEED) and a large effective Townsend coefficient (around 113 /mm as predicted by IMONTE). We show that the space charge field reaches the same magnitude as the applied electric field in avalanches at large gas gain. This strong space charge effect effectively suppresses large values for the avalanche charges. The shape of the simulated charge spectra is very similar to the measurements. Also the simulated average charges are close to the experimental results. RPCs are operated in a strong space charge regime over a large range of applied voltage, contrary to wire chambers. We apply only standard detector physics simulations to RPCs. The performance of Timing and Trigger RPCs is well reproduced by our simulations. The results concerning the space charge effect were presented and discussed at the 'RPC 2001' workshop [5] and on the '2002 NSS/MIC' conference [6].
This thesis presented the measurement of antideuteron and antihelium-3 production in central AuAu collisions at V SNN = 200 GeV center-of-mass energy at RHIC. The analysis is based on STAR data, about 3 x 10 high 6 events at top 10% centrality. Within the data sample a total number of about 5000 antideuterons and 193 antihelium-3 were observed in the STARTPC at mid-rapidity. The specific energy loss measurement in the TPC provides antideuteron identification only in a small momentum window, antihelium-3 however can be identified nearly background free with almost complete momentum range coverage. Following the statistical analysis of the hadronic composition at chemical freeze-out of the fireball, the antinuclei abundances were analyzed in terms of the same statistical description. Now applied to the clusterization of the fireball, the statistical analysis yields a fireball temperature of (135+-10) MeV and chemical potential of (5+-10) MeV at kinetic freeze-out. In the same way as the hadronization, the clusterization process is phase-space dominated and clusters are born into a state of maximum entropy. The large sample of observed antihelium-3 allowed for the first time in heavy-ion physics to calculate a differential multiplicity and invariant cross section as a function of transverse momentum. As expected, the collective transverse flow in the fireball flattens the shape of the transverse momentum spectrum and leads to the high inverse slope parameter of (950+-140) MeV of the antihelium-3 spectrum. With the extracted mean transverse momentum of antihelium-3, the collective flow velocity in transverse direction could be estimated. As the average thermal velocity is small compared to the mean collective flow velocity for heavy particles, the mean transverse momentum of antihelium-3 by itself constrains the flow velocity. Here, a simple ideal-gas approximation was fitted to the distribution of the mean transverse momentum as a function of particle mass and provided direct access to the kinetic freeze-out temperature and the flow velocity. A concept, which is complementary to the combined analysis of momentum spectra and two-particle HBT correlation methods commonly used to extract these parameters, and a cross check for the statistical analysis. The upper limit for the transverse collective flow velocity from the antihelium-3 measurement alone is v flow <= (0.68+-0.06)c, whereas the ideal-gas approximation yields a temperature of (130+-40) MeV and v flow = (0.46+-0.08)c. The results indicate, that the kinetic freeze-out conditions at SPS and RHIC are very similar, except for a smaller baryon chemical potential at RHIC. The simultaneous inclusive measurement of antiprotons allowed to study the cluster production in terms of the coalescence picture. With the large momentum coverage of the antihelium-3 momentum spectrum, the coalescence parameter could be calculated as a function of transverse momentum. Due to the difference between antiproton and antihelium-3 inverse slopes, increases with increasing transverse momentum - again a direct consequence of collective transverse flow. Both B2 and B3 follow the common behavior of decreasing coalescence parameters as a function of collision energy. According to the simple thermodynamic coalescence model, this indicates an increasing freeze-out volume for higher energies and is confirmed by the interpretation of the coalescence parameters in the framework of Scheibl and Heinz. Their model includes a dynamically expanding source in a quantum mechanical description of the coalescence process and expresses the coalescence parameter as a function of the homogeneity volume V hom accessible also in two-particle HBT correlation analyzes. The values for the antideuteron and antihelium-3 results agree well with the homogeneity volume from pion-pion correlations, but do not seem to follow the same transverse mass dependence. A comparison with proton-proton correlations may clarify this point and provide an important cross check for this analysis. Compared to SPS the homogeneity volume increases nearly by a factor of two. The analysis of the antinuclei emission at RHIC allowed to study the kinetic freeze-out of the created fireball. The results show, that the temperature and mean transverse velocity in the expanding system does not change significantly, when the collision energy increases by one order of magnitude. Only the source volume, i.e. the homogeneity volume, increases. That leaves open questions for the theoreticians to the details of the system evolution from the initial hot and dense phase - the initial energy density is a factor of two to three higher at RHIC than at SPS - to the final kinetic freeze-out with similar conditions. At the same time, the results are important constraints for the theoretical descriptions. The successful implementation of the Level-3 trigger system in STAR opens the door for the measurement of very rare signals. Indeed, in the coalescence physics perspective, the first observations of anti-alpha 4 He nuclei and antihypertritons 3/Delta H will come within the reach of STAR, in addition to a high statistics sample of antihelium-3.
Vascular occlusive diseases are one of the leading mortality causes in westernised countries. Occlusions of one of the major arteries can be overcome without devastating consequences provided a timely induction of compensating collateral arteries occurs. Perhaps the most outstanding feature of collateral vessel growth is the proliferation of smooth muscle cells (SMCs). Understanding the molecular mechanisms and identifying key molecular players of SMC proliferation would contribute significantly to the development of efficient therapies to intervene with all processes involving neointima formation, including collateral growth. mRNA and protein coding for co-transcription factor Egr1 were found to be up-regulated in growing collateral vessels 6, 12 or 24 hours following femoral artery ligation in mice. Since Egr1 is required for SMC proliferation in vitro and in vivo and likely to be implicated in the initiation of collateral artery growth, the key signalling mediators regulating Egr1 expression specifically in proliferating vascular SMCs were investigated. Northern blot and Western blot analysis revealed a strong up-regulation of Egr1 within 2 hours of stimulation with PDGF-AB and FGF-2. These two potent SMC mitogens involved in neointima formation were used to stimulate vascular SMCs not only to delineate the regulators of Egr1 expression but also to identify additional key mediators of SMC proliferation. FGF-2 but not PDGF-AB led to a drastic reduction of desmin amount in proliferating SMCs, correlating closely with the phenotypic modulation of SMCs in vivo. Both growth factors triggered a dramatic increase in DNA-synthesis rate with a concomitant loss of p27 exp Kip1. Stimulation with PDGF-AB and FGF-2 triggered a rapid and transient activation of PDGFRβ and FGFR1 respectively, thus providing the basis for activation of down-stream targets. Analysis of an array of signalling pathways demonstrated a strong activation of the Ras-Raf-MEK-ERK cascade in response to both factors as measured by the level of phosphorylation of prominent members MEK, ERK1/2 and c-Myc. SAPK/JNK and p38, which also belong to the superfamily of MAP kinases, did not become activated following stimulation with either PDGF-AB or FGF-2. The analysis of various PKC isoforms identified PKCδ and PKCθ to be the key mediators of PDGF-AB- and FGF-2-induced mitogenesis in proliferating SMCs. Whereas PDGF-AB potently stimulated PKB/Akt with concomitant GSK3β phosphorylation, FGF-2-induced inactivation of GSK3β was independent of PKB/Akt. Specific inhibition in order to evaluate the contribution of individual pathways to Egr1 expression and vascular SMC proliferation revealed that inhibition of the Raf-MEK-ERK module by UO126 completely abolished DNA-synthesis and Egr1 expression without a compensation by alternative pathways. Surprisingly, inhibition of PI3K led to a switch to the mitogenic RafMEK-ERK signalling cascade which resulted in an augmented Egr1 expression. In conclusion, in porcine vascular SMCs, activation of the Ras-Raf-MEK-ERK signalling module appears to be the main prerequisite for Egr1 expression and DNA synthesis induction in response to PDGF-AB and FGF-2 whereas related kinases SAPK/JNK and p38 play no significant role. Inhibition of the PI3K-Akt cascade represents an alternative way to activate ERK1/2 and induce Egr1 expression. Whereas MEK is the central regulator of mitogenic effects in proliferating vascular SMCs, the PI3K-Akt pathway most likely exerts survival function. Inactivation of MEK by its specific inhibitors identified hyperphosphorylation as ayet unknown mechanism of kinase inhibition.
Hepatitis E virus (HEV) is a positive-stranded RNA virus with a 7.2 kb genome that is capped and polyadenylated. The virus is currently unclassified : the organisation of the genome resembles that of the Caliciviridae but sequence analyses suggest that it is more closely related to the Togaviridae. HEV is an enterically transmitted virus that causes both epidemics and sporadic cases of acute hepatitis in many countries of Asia and Africa but only rarely causes disease in more industrialised countries. Initially the virus was believed to have a limited geographical distribution. However, serological studies suggest that that HEV may be endemic also in the United states and Europe even though it infrequently causes overt disease in these countries. Many different animal species worldwide recently have been shown to have antibodies to HEV suggesting that hepatitis E may be zoonotic. Although two related strains have been experimentally transmitted between species, direct transmission from animal to a human has not been documented. Our main objective in this study is to evaluate the suitability of current available HEV antibody assays for use in low-endemicity areas such as in Germany. Methods: We selected sera on the basis of at least borderline reactivity in the routinely used Abbot EIA. Most were tested as part of routine screening of long-term expatriates in endemic countries. The following assays (recombinant antigens : ORF2 and ORF3) were used: Abbot EIA, Genelabs ELISA, Mikrogen recomBlot and a 'Prototype' DSL-ELISA. We observed a wide range of sensitivity ( average of 56.8%) and specificity ( an average of 61.4%) in these used assays. These results implies that , these assays might be unreliable for detection of HEV infection in areas where hepatitis E is not endemic. However, most anti- HEV assays have not been correlated with the HEV RNA determined by reverse transcription. Many of these unexpected results and discrepancies can be alluded to the following reasons: I. The choice and the size of the HEV antigen. II. Duration of the antibody persistence III. A cross reactivity with different agent IV. Due to geographic species V. A low sensitivity of the available assays. VI. And infection with non-pathogenic HEV strain. (zoonotic strain?). We therefore suggest that, further studies will be required to improve the sensitivity and specificity of the available commercial assays on the market.
A gene trap strategy was used to identify genes induced in hematopoietic cells undergoing apoptosis by growth factor withdrawal. IL-3 dependent survival of hematopoietic cells relies on a delicate balance between proliferation and apoptosis that is controlled by the availability of cytokines (Thompson, 1995; Iijima et al., 2002). From our previous results of gene trap assay, we postulated that transcriptionally activated antagonistic genes against apoptosis might actually block or delay cell death (Wempe et al., 2001) causing cells to have carcinogenic behavior. The analysis attempted to better understand the outcome of a death program following IL-3 deprivation and to identify those survival genes whose expression is affected by time dependent manner. As described in the chapter 4, there would be two major conclusions evident from the three separate experiments (Genetrap, Atlas cDNA array and Affymetrix chips): Firstly 56% of trapped genes, that are up-regulated by IL-3 withdrawal (28 of 50), are directly related to cell death or survival. Secondly, unlike most array technologies, gene trapping only selects for the transiently induced genes that is independent of pre-existing steady state mRNA levels. In regarding correlations of the genes with potential carcinogenesis, the pre-existing mRNA makes difficult to describe the unique characteristics of deregulated tumor tissue genes. For a joint project with Schering (Schering AG, Berlin), the genes of our GTSTs were examined. The first screen with custom array was used to look for whether the survival genes of our GTSTs are involved in various cancer cell lines, whilst the second screen with Matched Tumor/Normal Array was used to characterize if the selected seven genes (ERK3, Plekha2, KIAA1140, PI4P5Ka/g, KIAA0740, KIAA1036 and PEST domains) are transformation-related genes or not in different tumor tissues. Twenty-six genes were identified as either induced or repressed in one or more cell lines. Genetic information is expressed in complex and ever changing patterns throughout a life span of cells. A description of these patterns and how they relate to the tissue specific cancer is crucial for our understanding of the network of genetic interactions that underlie the processes of normal development, disease and evolution. The development of cancer and its progression is clearly a multiplex phenotype, as a function of time, involving dozens of primary genes and hundreds of secondary modifier genes. There would be a major conclusion evident from the three separate experiments (Genetrap, Affymetrix mouse chip and Matched Tumor/Normal Array): ERK3 could play a significant role in breast, stomach and uterus carcinogenesis with tissue specific regulations. It is clear that ERK3 is obvious putative survival gene in these tumor tissues. Especially, in breast tumors, seven times up-regulation was considerable and the activation of ERK3 could be a feature of breast tumors. My results imply that the unique deregulation of ERK3 is perhaps the major consequence of possible transformation of normal cells into malignant cancer cells, even though further analysis remains to be determined whether an alterated activity of associated survival genes is primarily responsible for a carcinogenesis. However unlike all the other known MAP Kinases, no stimuli and no nuclear substrates of ERK3 is reported. Therefore, it will be necessary first to determine the spectrum of substrates and to identify the proximal effectors for the ERK3 in breast carcinoma cells.
Obwohl Böden unzweifelhaft ein signifikanter Pool von organischem Kohlenstoff sind, ist ihre Bedeutung als potenzielle langfristige Senke für atmosphärischen Kohlenstoff keineswegs klar. Trotz bedeutender wissenschaftlicher Forschritte aus den letzten Jahren zur Klärung der Kohlenstoffdynamik in Böden gibt es nach wie vor offene Fragen insbesondere hinsichtlich der spezifischen geochemischen Mechanismen, die für die Stabilisierung organischen Kohlenstoffs in Böden verantwortlich sind. Vor diesem Hintergrund besteht ein wesentliches Ziel der vorliegenden Dissertation darin, in unterschiedlichen Bodentypen die Konzentration von organischem Kohlenstoff und Stickstoff sowie die mineralogische Zusammensetzung zu untersuchen, um Hinweise auf einen möglichen Einfluss der Tonmineralogie, der spezifischen Oberfläche und der Oxidkonzentration auf die Stabilisierung organischen Materials zu ermitteln. Die Ergebnisse sollen einen Beitrag dazu liefern, die Mechanismen der Fixierung organischer Substanz in Böden besser zu verstehen und das vorhandene Wissen hierüber zu erweitern. Hierzu wurden fünf verschiedene Bodenprofile aus Hessen mit unterschiedlicher mineralogischer Zusammensetzung untersucht. Um die Auswirkungen verschiedener physikalischer und geochemischer Faktoren auf den Gehalt organischer Substanz in den untersuchten Böden festzustellen, wurden folgende Parameter untersucht: -Tonmineralogie, -organische Kohlenstoff- und Stickstoff-Konzentrationen, -%-Kationensättigung, -spezifische Oberfläche, -dithionit- und oxalatlösliche Gehalte an Fe, Al und Mn. Anhand dieser Parameter wurden weiterführende statistische Analysen unter Verwendung der Statistiksoftware SPSS für Windows durchgeführt, um mögliche statistische Zusammenhänge aufzudecken, die für die Stabilisierung von organischem Kohlenstoff in den betrachteten Böden verantwortlich sind. Die im Rahmen der vorliegenden Dissertation ermittelten Ergebnisse zeigen, dass der Tonanteil und die Tonmineralogie der untersuchten Böden nur einen begrenzten Einfluss auf die Stabilisierung organischer Substanz haben. Weiterhin wird gezeigt, dass die in der Literatur propagierte Beziehung zwischen spezifischer Oberfläche und der Konzentration organischen Kohlenstoffs nicht auf alle Böden anwendbar ist. Die Ergebnisse deuten darauf hin, dass die Präsenz von amorphen Eisen- und Aluminiumoxiden der wichtigste Einflussfaktor für die Fixierung von organischem Material in den untersuchten Böden ist. Die größeren Konzentrationen von organischem Kohlenstoff in den kleinsten Fraktionen (Feinschluff und Ton) der Profile sind vor allem darauf zurückzuführen, dass Oxide ebenfalls in diesen Fraktionen aufzufinden sind. Tonminerale haben demnach eine sekundäre Bedeutung, indem sie Komplexe mit den Oxiden bilden, die zur Stabilisierung von organischer Substanz führen können. Insgesamt deuten die Ergebnisse daraufhin, dass Böden keine geeignete Senke für die langfristige Speicherung von organischem Kohlenstoff sind. Obwohl Mechanismen wie die Adsorption von organischer Substanz an Oxide die Stabilisierung organischen Materials unterstützen, scheinen diese nicht stark genug zu sein, um eine permanente Speicherung von organischem Kohlenstoff zu bewirken.
The focus of this study were Celtic gold coins excavated from the Martberg, a Celtic oppidium and sanctuary, occupied in the first century B.C. by a Celtic tribe known as the Treveri. These coins and a number of associated coinages, were characterised in terms of their alloy compositions and their geochemical and isotopic signatures so as to answer archaeological and numismatic questions of coinage development and metal sources. This required the development of analytical methods involving; Electron Microprobe (EPMA), Laser Ablation-ICP-MS, solution Multicollector-ICPMS and LA-MC-ICP-MS. The alloy compositions (Au-Ag-Cu-Sn) were determined by EPMA on a small polished area on the edge of the coins. A large beam size, 50µm (diameter), was used to overcome the extreme heterogeneity of these alloys. These analyses were shown to be representative of the bulk composition of the coins. The metallurgical development of the coinages was defined and showed that the earlier coinages followed a debasement trend, which was superceded by a trend of increasing copper at the expense of sliver while gold compositions remained stable. This change occurred with the appearance of the inscribed "POTTINA" coinage, Scheers 30/V. Two typologically different coinages, Scheers 16 and 18 ("Armorican Types") were found to have markedly different compositions which do not fit into the trends described above. A Flan for a gold coin, which may indicate the presence of a mint at the Martberg, was found to have an identicle weight and composition as the Scheers 30/I coins, which preceeded the majority of the coins found at the Martberg in the coin development chronology. The trace element anaylses were made by Laser Ablation-ICPMS using an AridusTM desolvating nebuliser to introduce matrix matched solution standards to calibrate the measurements, which were then normalised to 100%. Quantitative results were obtained for the following elements: Sc, Ti, Cr, Mn, Co, Ni, Cu, Zn, Se, Ru, Rh, Pd, Ag, Sb, Te, W, Ir, Pt, Pb, Bi. The remaining elements remain problematic as they produced incorrect standardisations mainly due to chemical effects in solution such as adsorption onto the beaker walls or oxidation : V, Fe, Ga, Ge, As, Mo, Sn, Re, Os, Hg. Changes in the sources of Au, Ag and Cu were observed during the development of the coinages through the variation of trace elements, which correlate positively with the major components of the coin alloys. Changes in the Pt/Au ratios show that the Scheers 23 coins contain distinctly different gold from the later coinages and that the Scheers 18 gold source was also different. Te/Ag was used to show that the Sch.23 coins also contained different silver and some subgroups were observed in the Sch. 30/V coins. A major change in copper source is indicated by the sudden increase of Sb and Ni with the introduction of the Sch. 30/V coins (POTTINA), which can be linked to a similar change in copper observed in the contemporary silver coinage, Sch. 55 (with a ring). Lead isotopic analyses were made by solution- and Laser Ablation - MC-ICP-MS, The laser technique proved to be in good agreement with the solution analyses with precisions between 1 and 0.1%o (per mil). The development of the laser method opens the way for easy and virtually non-destructive Pb isotopic determinations of ancient gold coins. The results showed that Sch. 23 is very different from the following coinages, Sch. 16 and 18 are also different, forming their own group, and all the later "Eye" staters (Sch. 30/I-VI) lie on a mixing line controlled by the addition of copper from a Mediterranean source, probably Sardinia or Spain. An indication of gold and silver sources should be possible with further analyses of the Sch. 23 and Rainbow Cup gold coins and the Sch. 54 and 55 silver coinages. Copper Isotopic analyses were made by solution- and Laser Ablation - MC-ICP-MS. Both techniques require further development to produce more reproducible results. The results show that there appears to be a trend to more positive d Cu65 values for the later coinages and that the link between the copper used in the Sch. 30/V (POTTINA) coins and the silver Sch. 55 (with a ring) coins is also shown by similarly postive d Cu65 values. The full suite of analyses were also made on samples of gold from the region. They were mostly composed of "placer gold", alluvial gold found in rivers. It was found that when a study is restricted to a limited number of deposits or areas then it is possible to distinguish between deposits based on the concentration of those elements which are least affected by transport related alteration processes. These elements include; the PGE's, due to their refractory nature, and those elements which are usually present in high enough concentrations to remain relatively unaffected, eg: Cu, Pb and Sb. Due to the nature of the coin alloy it is not possible to link the gold used in the coins studied here with gold deposits, as the large amounts of Ag and Cu, added to the coin alloys, have masked the Au signature. However, further Pb isotopic analyses of gold deposits should prove useful in determining from which regions Celtic gold was derived.
One of the known apoptotic pathways in mammalian cells involves release of mitochondrial Cytochrome c into the cytosol. Cyt c then together with ATP or dATP induces a conformational change in the adaptator protein Apaf-1 (a homologue of the C. elegans CED4 protein) (Zou, Henzel et al. 1997), leading to its oligomerization and the recruitment of several pro-Casp-9 molecules. This protein complex assembly called "apoptosome" leads to the activation of Casp-9 which then initiates or amplifies the caspase cascade. The cell death program can be stalled at several points and we were interested in identifying new proteins inhibiting cell death downstream of Cyt c release. This thesis describes how I have screened a cDNA library derived from a pool of human breast carcinomas in a yeast-based survival screen, using the S. pombe yeast strain HC4 containing an inducible CED4 construct(James, Gschmeissner et al. 1997). The screen resulted in the identification of six proteins displaying cell death-inhibiting activity in S. pombe as well as anti-apoptotic potential in mammalian cells. Those six molecules were RoRet (Ruddy, Kronmal et al. 1997), Aven (Chau, Cheng et al. 2000), Fte-1/S3a (Kho, Wang et al. 1996), PGC2 (Padilla, Kaur et al. 2000; Goetze, Eilers et al. 2002), SAA1-2ß (Moriguchi, Terai et al. 2001) and FBP (Brockstedt, Rickers et al. 1998) of which I selected RoRet, Aven and Fte-1/S3a for further analysis. RoRet is a new anti-apoptotic molecule that can inhibit the mitochondrial pathway via its PRY-SPRY domain. RoRet does not seem to bind to Apaf-1, and does not co-localize with the activated Apaf-1/Caspase-9 complex. Aven was published to act as an anti-apoptotic protein and suggested to function via the recruitment of Bcl-XL to Apaf-1. This work shows that its C-terminal domain can bind to Apaf-1 and has a strong anti-apoptotic activity by itself. Moreover, Aven co-localizes with the activated Apaf-1/Caspase-9 complex suggesting that it is a component of the apoptosome. Furthermore, the expression of Aven is regulated in mammary glands during the pregnancy cycle. Fte-1/S3a has been already implicated in increased transformation capacity of v-Fos in fibroblasts (Kho and Zarbl 1992; Kho, Wang et al. 1996). This work shows that it has anti-apoptotic activity and can protect against Bak- and Apaf-1-induced apoptosis. It can bind directly to activated Apaf-1 at the linker domain between the WD40 repeats and the CED4-like domain, suggesting that it may protect by sequestering the activated Apaf-1 to some organelles whose nature remains to be determined. Moreover, expression studies on mRNA and protein level showed upregulation of Fte-1/S3a in colon, lung and kidney carcinoma. Hmgb1 (Flohr, Rogalla et al. 2001; Pasheva, Ugrinova et al. 2002; Stros, Ozaki et al. 2002) was identified during a survival screen performed with a NIH 3T3 mouse fibroblast cDNA library in a Bak-expressing yeast S. pombe strain. HMGB1 can protect against Bak-, UV-, FasL- and TRAIL-induced apoptosis. Significant overexpression of HMGB1 was found in breast and colon carcinoma, and elevated mRNA amounts were detected in uterus, colon and stomach carcinoma, suggesting that it may be a tumour marker (Brezniceanu et al., 2003).
In summary, the cooled heavy-ion beams of the ESR storage ring offer excellent experimental conditions for a precise study of the effects of QED in the groundstate of high-Z one- and two-electron ions. This has been demonstrated within the series of experiments conducted at the electron cooler device as well as at the gasjet target. In this work we have used a recently developed experimental approach to obtain the first direct measurement of the two-electron contributions to the ground state binding energy of helium-like uranium. By employing our method, all one-electron contributions to the binding energy such as finite-nuclear size corrections and the one-electron self energy cancel out completely. Note, this is a distinctive feature of this particular kind of QED test and is in contrast to all other tests of bound state QED for high-Z ions such as 1s Lamb shift (in one-electron systems), g-factor of bound electrons, or hyperfine splitting. Compared to former investigations conducted at the superEBIT in Livermore we could already substantially improve the statistical accuracy and extend studies to the higher-Z regime. Moreover, our result has reached a sensitivity on specific two-electron QED contributions. Our value agrees with the theoretical predictions within the experimental uncertainty. Similar to the superEBIT experiment possible sources of systematic errors are essentially eliminated and the final result is limited only by counting statistics. For the case of the 1s Lamb shift in hydrogen-like uranium, the achieved accuracy of +- 4.2 eV is a substantial improvement by a factor of 3 compared to the most precise value up to now [44] (see Fig. 5.6). Our result already provides a test of the first-order QED contributions at the 1.5% level and only a slight improvement is required in order to achieve a sensitivity to QED contributions beyond first-order SE and VP.