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Results are presented on Omega production in central Pb+Pb collisions at 40 and 158 AGeV beam energy. Given are transverse-mass spectra, rapidity distributions, and total yields for the sum Omega+Antiomega at 40 AGeV and for Omega and Antiomega separately at 158 AGeV. The yields are strongly under-predicted by the string-hadronic UrQMD model and are in better agreement with predictions from a hadron gas models. PACS numbers: 25.75.Dw
System size and centrality dependence of the balance function in A + A collisions at √sNN = 17.2 GeV
(2004)
Electric charge correlations were studied for p+p, C+C, Si+Si and centrality selected Pb+Pb collisions at sqrt s_NN = 17.2$ GeV with the NA49 large acceptance detector at the CERN-SPS. In particular, long range pseudo-rapidity correlations of oppositely charged particles were measured using the Balance Function method. The width of the Balance Function decreases with increasing system size and centrality of the reactions. This decrease could be related to an increasing delay of hadronization in central Pb+Pb collisions.
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.
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.
The cytochrome bc1 complex or ubiquinol:cytochrome c oxidoreductase (QCR) catalyses electron transfer from ubiquinol to cytochrome c in respiration and photosynthesis coupled to a vectorial proton transport across the membrane, in which the enzyme resides. In both bacteria and eukaryotic organisms, QCR participates in supramolecular assembly of membrane proteins that comprise the respiratory or photosynthetic chain. In the present work, proton transfer pathways, substrate binding and the supramolecular assembly of the respiratory chain in yeast were probed by structure-based site-directed mutagenesis and characterization of the variants. Both active sites centre P, the place of quinol oxidation, and centre N, where quinone reduction takes place, lack direct access to the bulk solvent necessary for proton release and uptake. Based on the X-ray structure, proton transfer pathways were postulated. Analysis at centre P showed, that E272 and Y132 of cytochrome b are important for QCR catalysis as indicated by increased superoxide production and lowered Cyc1p reductase activity in these variants. Pre-steady state heme reduction kinetics in combination with stigmatellin resistance indicated that charge and length of the side chain at position 272 are crucial for efficient docking of the ISP to form the enzyme substrate complex and for electron bifurcation at centre P. Variants of Y312 and F129, both residues of cytochrome b, showed an increased Km indicating participation of these residues in coordination of ubiquinol or the possible intermediate semiquinone anion radical. F129 proved to be crucial for a functional Q-cycle as indicated by respiratory negative growth phenotype and a lowered H+/e- stoichiometry of F129 variants. At centre N, the postulated CL/K and E/R proton transfer pathways are located at opposite sites of the bound ubiquinone. Variants in the surface residues R218 (cytochrome b) and E52 (Qcr7) of the E/R pathway and E82 (Qcr7) of the CL/K pathway showed instability upon purification indicating an important role of these residues for QCR integrity. The slowed down centre N reduction kinetics in H85 (CL/K), R218 and N208 (both E/R) variant was attributed to a destabilised semiquinone anion consistent with the observed decreased sensitivity towards the site-specific inhibitor antimycin and an increased Km. Variants of residues of both pathway, E82Q and R218M, exhibited a decreased H+/e- stoichiometry indicating a crucial role of both residue for maintaining a working Q-cycle and supporting the proposed protonation of the substrate via the Cl/K and the E/R pathway. Long-range interaction between centre N and centre P were observed by altered reduction kinetics of the high potential chain and increased superoxide production in the centre N variants. The role of the cation-pi-interaction between F230 of Cyt1p and R19 of cytochrome c in binding of the redox carrier to QCR was analysed. In F230L hydrophobic interaction were partially lost as was deduced from the ionic strength dependence of Cyc1p reductase activity and Cycp1 binding, as detected by ionic strength sensitive Kd and Km for Cyc1p. The decreased enzymatic rate of F230W could be explained by a disturbed binding of Cyc1p to the variant enzyme. F230 may influence the heme mid point potential and thereby the electron transfer rate to Cyc1p. Reduction of Cobp via both centre P and centre N was disturbed suggesting an interaction between high and low potential chain. Supramolecular association between QCR and cytochrome c oxidase (COX) in yeast mitochondria was probed by affinity chromatography of a his-tagged QCR in the presence of the mild detergent digitonin. In comparison to purification with laurylmaltoside, the presence of both QCR and COX subunits was detected in the elution fractions by SDS-PAGE, Cyc1p reductase and TMPD oxidase activity assays and immunoblot analysis. The CL-dependent formation of the supercomplex between QCR and COX was analysed by replacement variants in the CL-binding site of QCR in CL containing and CL free environment. With an increasing number of replacements of the three lysines the CL-binding pocket supercomplex formation was not abolished, when CL is present as shown by BN-PAGE analysis. This was supported by the synergetic decrease in enzyme activity for both enzymes upon increased number of replacements. In the CL-free environment, no supracomplex formation was observed for a wildtype CL binding site. By replacements of two lysines in the CL-binding pocket, supercomplex formation could be recovered as revealed by BN-PAGE. This indicates, that CL may serve as a charge neutralizer for the lysines near the presumed interaction domain between complex III and complex IV. The obtained results for centre P provide new information of residues critical for stabilisation of ubiquinol and controlling electron short circuit reactions. The observations for centre N variants clearly support the proposed two proton transfer pathways and the role of the bound phospholipids in centre N kinetics. Variants in the Cyc1p binding site suggest a role for F230 both in Cyc1p binding and electron transfer. Clear interaction between the high and low potential chain in both Cyt1p and centre N variants strongly support long-range interactions in the complex. Studies on the supramolecular association of complex III and complex IV indicate a new role of Cl in stabilising a supracomplex.