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Quantum Molecular Dynamics (QMD) calculations of central collisions between heavy nuclei are used to study fragment production and the creation of collective flow. It is shown that the final phase space distributions are compatible with the expectations from a thermally equilibrated source, which in addition exhibits a collective transverse expansion. However, the microscopic analyses of the transient states in the intermediate reaction stages show that the event shapes are more complex and that equilibrium is reached only in very special cases but not in event samples which cover a wide range of impact parameters as it is the case in experiments. The basic features of a new molecular dynamics model (UQMD) for heavy ion collisions from the Fermi energy regime up to the highest presently available energies are outlined.
The behavior of hadronic matter at high baryon densities is studied within Ultrarelativistic Quantum Molecular Dynamics (URQMD). Baryonic stopping is observed for Au+Au collisions from SIS up to SPS energies. The excitation function of flow shows strong sensitivities to the underlying equation of state (EOS), allowing for systematic studies of the EOS. Dilepton spectra are calculated with and without shifting the rho pole. Except for S+Au collisions our calculations reproduce the CERES data.
The behavior of hadronic matter at high baryon densities is studied within Ultrarelativistic Quantum Molecular Dynamics (URQMD). Baryonic stopping is observed for Au+Au collisions from SIS up to SPS energies. The excitation function of flow shows strong sensitivities to the underlying equation of state (EOS), allowing for systematic studies of the EOS. Effects of a density dependent pole of the rho-meson propagator on dilepton spectra are studied for different systems and centralities at CERN energies.
We study the thermodynamic properties of infinite nuclear matter with the Ultrarelativistic Quantum Molecular Dynamics (URQMD), a semiclassical transport model, running in a box with periodic boundary conditions. It appears that the energy density rises faster than T4 at high temperatures of T approx. 200 - 300 MeV. This indicates an increase in the number of degrees of freedom. Moreover, We have calculated direct photon production in Pb+Pb collisions at 160 GeV/u within this model. The direct photon slope from the microscopic calculation equals that from a hydrodynamical calculation without a phase transition in the equation of state of the photon source.
The microscopic phasespace approach URQMD is used to investigate the stopping power and particle production in heavy systems at SPS and RHIC energies. We find no gap in the baryon rapidity distribution even at RHIC. For CERN energies URQMD shows a pile up of baryons and a supression of multi-nucleon clusters at midrapidity.
Neben dem Erregernachweis beruht die Labordiagnose der Cytomegalie auf der Bestimmung HCMV spezifischer IgG-, IgM- und IgAAntikörper. Von der Industrie werden jedes Jahr neue Antikörpertests basierend auf der ELISA-Technologie angeboten. In der vorliegenden Studie wurden ein neues Testverfahren (Freka CMV-M-ELISA, Fresenius, Bad Homburg) mit bereits seit mehreren Jahren etablierten und zugelassenen ELISAs (Enzygnost CMVIgM; Behringwerke, Marburg und CMV-ELA, Medac, Hamburg) verglichen. Zur Bestimmung der Sensitivität wurden Verlaufsproben von 15 Organtransplantierten mit einer aktiven HCMV-Infektion, welche in den meisten Fällen über ein positives Ergebnis in der HCMV-DNA-PCR und/oder Virusisolierung und/oder quantitative pp65-Antigenbestimmung bestätigt wurde, untersucht. Zur Ermittlung der Spezifität wurde ein Kollektiv von bekannten HCMV-IgM-negativen Serumproben sowie potentiell kreuzreaktive Seren mit Antikörpern gegen andere Herpesviren und Rheumafaktor- bzw. Antinuklear-Antikörper-positive Seren untersucht. Die höchste Sensitivität wurde für den Medac-ELA ermittelt. Der Freka CMV-M ELISA zeigte eine ähnliche Sensitivität und Spezifität wie der Enzygnost CMV-IgM. Relativ zum Erregernachweis über PCR, Virusisolierung und quantitative pp65-Antigenbestimmung dauerte es bei vielen Patienten bis zu mehreren Wochen, ehe eine humorale Immunantwort über die Bildung von spezifischem IgM nachweisbar war. Bei zwei Patienten waren trotz dem Vorliegen einer floriden Cytomegalie keine HCMV-IgM-Antikörper bis zum Ende des Beobachtungszeitraums nachweisbar. Die Ergebnisse unserer Studie zeigen, daß es relativ große Unterschiede in bezug auf die Sensitivität der verschiedenen ELISAs gibt.
Microscopic calculations of central collisions between heavy nuclei are used to study fragment production and the creation of collective flow. It is shown that the final phase space distributions are compatible with the expectations from a thermally equilibrated source, which in addition exhibits a collective transverse expansion. However, the microscopic analyses of the transient states in the reaction stages of highest density and during the expansion show that the system does not reach global equilibrium. Even if a considerable amount of equilibration is assumed, the connection of the measurable final state to the macroscopic parameters, e.g. the temperature, of the transient "equilibrium" state remains ambiguous.
We analyze the reaction dynamics of central Pb+Pb collisions at 160 GeV/nucleon. First we estimate the energy density pile-up at mid-rapidity and calculate its excitation function: The energy density is decomposed into hadronic and partonic contributions. A detailed analysis of the collision dynamics in the framework of a microscopic transport model shows the importance of partonic degrees of freedom and rescattering of leading (di)quarks in the early phase of the reaction for E >= 30 GeV/nucleon. The energy density reaches up to 4 GeV/fm 3, 95% of which are contained in partonic degrees of freedom. It is shown that cells of hadronic matter, after the early reaction phase, can be viewed as nearly chemically equilibrated. This matter never exceeds energy densities of 0.4 GeV/fm 3, i.e. a density above which the notion of separated hadrons loses its meaning. The final reaction stage is analyzed in terms of hadron ratios, freeze-out distributions and a source analysis for final state pions.
In this paper, the concepts of microscopic transport theory are introduced and the features and shortcomings of the most commonly used ansatzes are discussed. In particular, the Ultrarelativistic Quantum Molecular Dynamics (UrQMD) transport model is described in great detail. Based on the same principles as QMD and RQMD, it incorporates a vastly extended collision term with full baryon-antibaryon symmetry, 55 baryon and 32 meson species. Isospin is explicitly treated for all hadrons. The range of applicability stretches from E lab < 100$ MeV/nucleon up to E lab> 200$ GeV/nucleon, allowing for a consistent calculation of excitation functions from the intermediate energy domain up to ultrarelativistic energies. The main physics topics under discussion are stopping, particle production and collective flow.
We perform an event-by-event analysis of the transverse momentum distribution of final state particles in central Pb(160AGeV)+Pb collisions within a microscopic non-equilibrium transport model (UrQMD). Strong influence of rescattering is found. The extracted momentum distributions show less fluctuations in A+A collisions than in p+p reactions. This is in contrast to simplified p+p extrapolations and random walk models.