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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].
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.
Die Entwicklung der Renormierungsgruppen-Technik, die in ihrer feldtheoretischen Version auf Ideen von Stückelberg und Petermann und in der Festkörperphysik auf K.G. Wilson zurückgeht, hat wesentliche Einsichten in die Natur physikalischer Systeme geliefert. Insbesondere das Konzept der so genannten Universalitätsklassen erhellt, warum Systeme, die durch scheinbar sehr verschiedene Hamilton-Operatoren beschrieben werden, doch im Wesentlichen die selbe (Niederenergie-)Physik zeigen. Ein weiterer Grund für den Erfolg dieser Methode liegt darin begründet, dass sie in systematischer Weise unendlich viele Feynman-Diagramme aufsummiert und somit über konventionelle Störungstheorie hinaus geht. Dies spielt in der Festkörperphysik vor allem dann eine wichtige Rolle, wenn das vorliegende physikalische System stark korreliert ist. Entsprechend der Vielzahl von Anwendungsmöglichkeiten hat sich in den vergangenen Jahrzehnten eine große Bandbreite verschiedener Formulierungen der Renormierungsgruppen-Technik ergeben. Eine davon ist die sogenannte funktionale Renormierungsgruppe, die auf Wegner und Houghton zurück geht und die auch in der vorliegenden Arbeit benutzt und weiter entwickelt wurde. Wir haben hier insbesondere auf die Einbeziehung der wichtigen Reskalierungsschritte wertgelegt. Als erstes Anwendungsgebiet des neu entwickelten Formalismus wurden stark korrelierte Elektronen in einer Raumdimension ausgewählt und hier insbesondere ein Modell, das als Tomonaga-Luttinger-Modell (TLM) bezeichnet wird. Im TLM wechselwirken Elektronen mit einer strikt linearen Energiedispersion ausschließlich über so genannte Vorwärtsstreu-Prozesse. Aufgrund der Linearisierung der Energiedispersion nahe der Fermipunkte ergibt sich ein Modell, das z.B. mit Hilfe der so genannten Bosonisierungs-Technik exakt gelöst werden kann. Hauptziel der vorliegenden Arbeit ist es, die bekannte Spektralfunktion dieses Modells unter Verwendung des Renormierungsgruppen-Formalismus zu reproduzieren. Gegenüber der bisherigen Implementierung der Renormierungsgruppe, bei der lediglich der Fluss einer endlichen Anzahl von Kopplungskonstanten betrachtet wird, stellt die Berechnung des Flusses ganzer Korrelationsfunktionen eine enorme Erweiterung dar. Der Erfolg dieser Herangehensweise im TLM bestärkt die Hoffnung, dass es in Zukunft auch möglich sein wird, die Spektralfunktionen anderer Modelle mit dieser Methode zu berechnen, bei denen herkömmliche Techniken versagen.
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.
Periplasmic Sud protein encoded by the Wolinella succinogenes catalyses the transfer of bound polysulfide-sulfur to the active site of the membrane bound polysulfide reductase. The homodimeric protein consists of 131 residues per monomer, each with one cysteine residue in the active site. Polysulfide-sulfur is covalently bound to the catalytic Cys residues of the Sud protein. In order to understand the structure-function relationship of this protein, the features of its solution structure determined by heteronuclear multidimensional NMR techniques are reported here. The first step of structure determination leads to resonance assignments using 15N/13C/2H- and 15N/13C-labeled protein. The sequential backbone and side chain resonance assignments have been successfully completed. Structure calculations were carried out using the ARIA program package. The structure is based on 2688 NOE-derived distance restraints, 68 backbone hydrogen bond restraints derived from 34 slow-exchanging backbone amide protons and 334 torsion angle restraints obtained from the TALOS program as well as 158 residual dipolar coupling restraints for the refinement of relative vector orientations. The three-dimensional structure of the Sud protein was determined with an averaged rootmean- square deviation of 0.72 Å and 1.28 Å for the backbone and heavy atoms, respectively, excluding the terminal residues. Without the poorly defined segment between residues 90-94 the average r.m.s.d. value drops down to 0.6 Å and 1.14 Å. The ensemble refined with residual dipolar coupling (rdc) restraints shows good convergence. The r.m.s.d. value for the backbone heavy atoms, excluding residues 90- 94, drops down from 0.97 to 0.66 for the rdc-refined ensemble. The relative orientation of the two monomers in the protein structures refined with residual dipolar coupling restraints are also different from those without residual dipolar coupling restraints. The structure determination of the dimeric protein has been hampered by the high molecular mass (30 kDa), severe peak degeneracy, and by the small number of experimental intermonomer NOEs (relative orientation problem of two monomers). For the resonance assignments of aliphatic side chain, many resonances were ambiguously assigned because of severe overlap of signals. The Sud dimer protein contains 17 Lys, 14 Leu and one His tag for each monomer. It complicated the resonance assignments. The conventional 3D 15N-separated TOCSY HSQC experiment failed because of the large molecular weight which results in line broadening and hence made the resonance assignments of side chains more difficult. The determined structure contains a five-stranded parallel ß-sheet enclosing a hydrophobic core, a two-stranded anti-parallel ß-sheet and seven a-helices. The dimer structure is stabilized predominantly by hydrophobic residues. Sud catalyses the transfer of the polysulfide-sulfur to cyanide, similar to rhodanese encoded by Azotobacter vinelandii (Bordo et al., 2000). The two proteins are similar in the active site environment primarily owing to the main-chain conformation of the active-site loop with the cysteine residue and with respect to the surrounding positively charged residues. The active-site loop (residues 89-95) in the Sud protein appears to be flexible, reflected by few assigned proton resonances of residues 90-94 in the active site. Despite their similarity in function and their similar structure in active site, the amino acid sequences and the folds of the two proteins are remarkably different. The negatively charged polysulfide interacts with positively charged R46, R67, and R94 and hence may be stabilized in structure. The mutation of one of the three arginines that are also conserved in rhodanese from A. vinelandii leads to a loss of sulfur-transfer activity. The polysulfide chain extends from inside of Sud protein to outside, where Sud may form contacts with polysulfide reductase. These contacts provide the possible polysulfide-sulfur transfer from Sud protein to the active site of polysulfide reductase.
Die Dissertation kombiniert die Methode der funktionellen Magnetresonanztomographie (fMRT) zur genauen räumlichen Lokalisation aufgabenkorrelierter parietaler Aktivierungen mit Transkranieller Magnetstimulation (TMS) zur systematischen Untersuchung der funktionellen Relevanz dieser Aktivierungen für die tatsächliche Leistungsfähigkeit. Die experimentelle Kombination beider Methoden ermöglichte die gezielte Stimulation der im tMRT identifizierten, mit visuospatialen Fähigkeiten assoziierten Hirnareale. Durch die systematische Auswertung der TMS-induzierten visuospatialen Leistungsveränderungen wurde die spezifische funktionelle Bedeutung dieser Hirnareale für visuospatiale Leistungen experimentell untersucht. Der zugrunde gelegte Versuchsplan umfasste sowohl visuospatiale Leistungen auf der Grundlage visuell dargebotener als auch mental vorgestellter Aufgaben. Dies ermöglichte die systematische Untersuchung, ob und inwieweit mentale visuospatiale Informationsverarbeitung die gleichen oder ähnliche Aktivierungsmuster im fMRT aufweist wie visuospatiale Verarbeitung visuell dargebotener Stimuli, und ob sich diese Aktivierungsmuster vorgestellter Stimuli unter dem Einfluss von rTMS in gleicher Weise als funktionell relevant erweisen. Aufgrund der separaten unilateralen Stimulation beider Hemisphären konnten darüber hinaus die unterschiedlichen behavioralen Auswirkungen einer Aktivierungsunterdrückung des linken und rechten Parietalkortex systematisch untersucht werden. Obwohl die Ausführung visuospatialer Aufgaben, sowohl auf der Grundlage visuell dargebotener als auch mental vorgestellter Stimuli, im fMRT mit einer bilateralen Aktivierung im Parietalkortex korrelierte, führte lediglich die TMS-induzierte temporäre Unterbrechung der neuronalen Aktivierung im rechten Parietalkortex zu einer signifikanten Verschlechterung in der Leistungsfähigkeit der damit assoziierten visuospatialen Aufgaben. Auf der Grundlage dieser Ergebnisse wurde ein modulares Modell der visuospatialen Imagination formuliert, in welchem den aufgabenkorrelierten bilateralen Aktivierungen aufgrund ihrer raum-zeitlichen Separierbarkeit unterschiedliche mentale Prozesse und aufgrund der mit TMS aufgezeigten funktionellen hemisphärischen Asymmetrie parietaler Aktivierung für visuospatiale Informationsverarbeitung unterschiedliche Kompensationsmechanismen zugeordnet wurden.