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System size dependence of multiplicity fluctuations of charged particles produced in nuclear collisions at 158 A GeV was studied in the NA49 CERN experiment. Results indicate a non-monotonic dependence of the scaled variance of the multiplicity distribution with a maximum for semi-peripheral Pb+Pb interactions with number of projectile participants of about 35. This effect is not observed in a string-hadronic model of nuclear collision HIJING.
The hadronic final state of central Pb+Pb collisions at 20, 30, 40, 80, and 158 AGeV has been measured by the CERN NA49 collaboration. The mean transverse mass of pions and kaons at midrapidity stays nearly constant in this energy range, whereas at lower energies, at the AGS, a steep increase with beam energy was measured. Compared to p+p collisions as well as to model calculations, anomalies in the energy dependence of pion and kaon production at lower SPS energies are observed. These findings can be explained, assuming that the energy density reached in central A+A collisions at lower SPS energies is sufficient to transform the hot and dense nuclear matter into a deconfined phase.
Results are presented from a search for the decays D0 -> K min pi plus and D0 bar -> K plus pi min in a sample of 3.8x10^6 central Pb-Pb events collected with a beam energy of 158A GeV by NA49 at the CERN SPS. No signal is observed. An upper limit on D0 production is derived and compared to predictions from several models.
Low energy beam transport (LEBT) for a future heavy ion driven inertial fusion (HIDIF [1]) facility is a crucial point using a Bi+ beam of 40 mA at 156 keV. High space charge forces (generalised perveance K=3.6*10-3) restrict the use of electrostatic focussing systems. On the other hand magnetic lenses using space charge compensation suffer from the low particle velocity. Additionally the emittance requirements are very high in order to avoid particle losses in the linac and at ring injection [2]. urthermore source noise and rise time of space charge compensation [3] might enhance particle losses and emittance. Gabor lenses [4] using a continuous space charge cloud for focussing could be a serious alternative to conventional LEBT systems. They combine strong cylinder symmetric focussing with partly space charge compensation and low emittance growth due to lower non linear fields. A high tolerance against source noise and current fluctuations and reduced investment costs are other possible advantages. The proof of principle has already been shown [5, 6]. To broaden the experiences an experimental program was started. Therefrom the first experimental results using a double Gabor lens (DGPL, see fig. 1 ) LEBT system for transporting an high perveance Xe+ beam will be presented and the results of numerical simulations will be shown.
Rapidity distributions for Lambda and anti-Lambda hyperons in central Pb-Pb collisions at 40, 80 and 158 AGeV and for K 0 s mesons at 158 AGeV are presented. The lambda multiplicities are studied as a function of collision energy together with AGS and RHIC measurements and compared to model predictions. A different energy dependence of the Lambda/pi and anti-Lambda/pi is observed. The anti-Lambda/Lambda ratio shows a steep increase with collision energy. Evidence for a anti-Lambda/anti-p ratio greater than 1 is found at 40 AGeV.
Die vorliegende Arbeit hat es sich zur Aufgabe gemacht, mit der Themenstellung "Netzaktivismus" eine relativ aktuelle Entwicklung aufzugreifen. Als nötig erschien mir hierbei von vornherein, den eigentlichen Kontext des Netzaktivismus, das Internet, einigermaßen genau in den Blick zu bekommen. Ursprünglich war also vorgesehen, zur Einleitung die militärgeschichtliche Herkunft des Internet zu klären und zu bewerten, um dann, anhand der Genese des Internet zu einem Massenmedium unter dem Stichpunkt "Gegenwärtige Nutzungsformen des Internet" der Frage nach der Faszination an diesem neuen Medium nachzugehen. Herausfinden wollte ich dabei, ob die Nutzer sich vornehmlich aktiv oder passiv an dem neuen Medium beteiligen und ob die "Aktivitäten", um die es schließlich in meiner Arbeit geht, überhaupt eine Relevanz für den Großteil der Internetnutzer hat. Dies stellte sich aber als schwieriger heraus, als erwartet. So kann auch in dieser Arbeit wenig darüber gesagt werden, warum denn das Internet in der Gegenwart eine so wichtige Rolle zu spielen scheint. An gegebener Stelle wird noch darauf zurückzukommen sein.
Die Dokumente enthalten jeweils die gleiche Arbeit, allerdings in drei unterschiedlichen Varianten, die sich in der Qualität der Bilder und damit in der Filegröße unterscheiden: * Bilder in voller Druckqualität (8,2 MB): DissWFOM1.pdf (Dokument1) * Photos in reduzierter Auflösung (3,1 MB): DissWFOM2.pdf (Dokument2) * Photos und Zeichnungen in red. Auflösung (1,4 MB): DissWFOM3.pdf (Dokument3)
Cold target recoil ion momentum spectroscopy (COLTRIM) has been employed to image the momentum distributions of continuum electrons liberated in the impact of slow He2+ on He and H2. The distributions were measured for fully determined motion of the nuclei that is as a function of the impact parameter and in a well de ned scattering plane The single ionization (SI) of H2 leading to H2+ recoil ions in nondissociative states (He2+ + H+ -> He2+ + H+ + e-) and the transfer ionization (TI) of H2 leading to H2 dissociation into two free protons (He2+ H2 -> He+ + H+ + H+ + e-) were investigated. Similar measurements have been carried out for He target, the corresponding atomic two electron system, i.e. the single ionization (SI) (He2+ + He -> He+ + He2+ e- and the transfer ionization (TI) (He2+ + He -> He+ + He2+ + e-). These measurements have been exploited to understand the results obtained for H target. In comparing the continuum electron momentum distributions for H2 with that for He, a high degree of similarity is observed. In the case of transfer ionization of H2, the electron momentum distributions generated for parallel and perpendicular molecular orientations revealed no orientation dependence. The in scattering plane electron momentum distributions for the transfer ionization of H2 by He2+ and for the transfer ionization of He by He2e showed that the salient feature of these distributions for both collisions systems consists in the appearance of two groups of electrons with difeerent structures. In addition to the group of the saddle electrons forming two jets separated by a valley along the projectile axis we nd a new group of electrons moving with a velocity higher than the projectile velocity These new fast forward electrons result from a narrow range of impact parameters and appear as image saddle in the projectile frame. In contrast to the transfer ionization of He, the fast forward electrons group disappears in the in scattering plane electron momentum distribution generated for the single ionization of He. Instead of this group another new group of electrons appear These electrons exhibit an amount of backscattering These backward elec trons appear as image saddle in the target frame The structures that the saddle electrons show are owing to the quasi molecular nature of the collision process For the TI of H2, the TI of He and the SI of He, a pi-orbital shape of the electron momentum distribution is observed This indicates the importance of the rotational coupling 2-p-theta -> 2p-pi in the initial promotion of the ground state followed by further promotions to the continuum The backward electrons as well as the fast forward electrons are not discussed in the theoretical literature at all. However, a number of obvious indications of the existence of the backward and fast forward electrons could be seen in the experimental works of Abdallah et al. as well as in the theoretical calculations of Sidky et al One might speculate that electrons which are promoted on the saddle for some time during the collision could finally swing around the He+ ion in the way out of the collision, i.e. either around the projectile in the forward direction as in the TI case forming the fast forward electrons or around the recoil ion in the backward direction as in the SI case forming the backward electrons. This might be a result of the strong gradient, and hence the large acceleration of the screened He+ potential.
The cytochrome bc1 complex is a cornerstone in bioenergetic electron transfer chains, where it carries out tasks as diverse as respiration, photosynthesis, and nitrogen fixation. This homodimeric multisubunit membrane protein has been studied extensively for several decades and the enzyme mechanism is described with the modified protonmotive Q cycle. Still, the molecular and kinetic description of the catalytic cycle is not complete and questions remain regarding the bifurcation of electron transfer at the quinol oxidation (Qo) site, substrate occupancy, pathways of proton conduction, and the nature of the Rieske protein domain movement. We used competitive inhibitors to study the molecular architecture at the Qo site with X-ray crystallography. The structure of the enzyme with the substrate analog 5-n-heptyl-6-hydroxy-4,7-dioxobenzothiazole (HHDBT) bound at the Qo site was determined at 2.5 Å resolution. Spectroscopic studies showed that HHDBT is negatively charged when bound at the active site. Mechanistic interpretations from inhibitor binding are in line with single occupancy model for quinol oxidation and structural analysis supports the proposed proton transfer pathway. For functional insight into the enzyme mechanism, redox-sensitive protonation changes were studied by Fourier transform infrared spectroscopy. The protein purification procedure was optimized for less delipidation and the isolated enzyme was more active. Furthermore, two new phospholipids were identified in the X-ray structures, including a cardiolipin. Strikingly, conserved lipid binding cavities were observed in structural comparison with homologous enzymes. The functional role of tightly bound phospholipids will be discussed. Finally, the Qo site is a target for various compounds of agricultural and pharmaceutical importance. Importantly, the X-ray structures permit detailed analysis of the molecular reasons for acquired resistance to and treatment failure of Qo site inhibitors, such as atovaquone, that is used to treat malaria and pneumonia, as discussed herein.