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Signatures of dense hadronic matter in ultrarelativistic heavy ion reactions
(1996)
- 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.
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Relativistic hadron-hadron collisions in the ultra-relativistic quantum molecular dynamics model
(1999)
- Hadron-hadron collisions at high energies are investigated in the Ultra- relativistic-Quantum-Molecular-Dynamics approach. This microscopic trans- port model describes the phenomenology of hadronic interactions at low and intermediate energies ( s < 5 GeV) in terms of interactions between known hadrons and their resonances. At higher energies, s > 5 GeV, the excitation of color strings and their subsequent fragmentation into hadrons dominates the multiple production of particles in the UrQMD model. The model shows a fair overall agreement with a large body of experimental h-h data over a wide range of h-h center-of-mass energies. Hadronic reaction data with higher precision would be useful to support the use of the UrQMD model for relativistic heavy ion collisions.
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Reaction dynamics in Pb+Pb at the CERN/SPS: from partonic degrees of freedom to freeze-out
(1998)
- 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.
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Physics opportunities at RHIC and LHC
(1999)
- Nonequilibrium models (three-fluid hydrodynamics, UrQMD, and quark molecular dynamics) are used to discuss the uniqueness of often proposed experimental signatures for quark matter formation in relativistic heavy ion collisions from the SPS via RHIC to LHC. It is demonstrated that these models - although they do treat the most interesting early phase of the collisions quite differently (thermalizing QGP vs. coherent color fields with virtual particles) -- all yield a reasonable agreement with a large variety of the available heavy ion data. Hadron/hyperon yields, including J/Psi meson production/suppression, strange matter formation, dileptons, and directed flow (bounce-off and squeeze-out) are investigated. Observations of interesting phenomena in dense matter are reported. However, we emphasize the need for systematic future measurements to search for simultaneous irregularities in the excitation functions of several observables in order to come close to pinning the properties of hot, dense QCD matter from data. The role of future experiments with the STAR and ALICE detectors is pointed out.
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Nucleus-nucleus collisions at highest energies
(1996)
- 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.
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Microscopic models for ultrarelativistic heavy ion collisions
(1998)
- 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.
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Microscopic calculations of stopping and flow from 160AMeV to 160AGeV
(1996)
- 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.
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Microscopic analysis of thermodynamic parameters from 160 MeV/n - 160 GeV/n
(1997)
- 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.
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Local thermodynamical equilibrium and the equation of state of hot, dense matter created in Au+Au collisions at AGS
(1998)
- Local kinetic and chemical equilibration is studied for Au+Au collisions at 10.7 AGeV in the microscopic Ultrarelativistic Quantum Molecular Dynamics model (UrQMD). The UrQMD model exhibits dramatic deviations from equilibrium during the high density phase of the collision. Thermal and chemical equilibration of the hadronic matter seems to be established in the later stages during a quasiisentropic expansion, observed in the central reaction cell with volume 125 fm3. For t > 10 fm/c the hadron energy spectra in the cell are nicely reproduced by Boltzmann distributions with a common rapidly dropping temperature. Hadron yields change drastically and at the late expansion stage follow closely those of an ideal gas statistical model. The equation of state seems to be simple at late times: P = 0.12 Epsilon. The time evolution of other thermodynamical variables in the cell is also presented.
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Identifizierung und Charakterisierung der mRNA processing bodies von Arabidopsis thaliana
(2007)
- mRNA-Abbau ist ein essentieller Prozess der Genexpression, der den Zellen ermöglicht, die Qualität und die Quantität der mRNA zu kontrollieren. Besonders unter Stressbedingungen könnte der mRNA-Abbau eine bedeutende Rolle neben der Speicherung von mRNAs sowie der Regulation der Proteinhomöostase zum Schutz vor schädigenden Einflüssen spielen. Studien mit Hefen und Säugerzellen zeigten, dass dem 5'-3'mRNA-Abbau ein wichtige Rolle sowohl unter normalen Bedingungen als auch unter Stressbedingungen zukommt und dieser in zytoplasmatischen Processing bodies (P-bodies) stattfindet. Im Rahmen dieser Arbeit sollten Erkenntnisse über den 5'-3'mRNA-Abbau erhalten werden. Im Vordergrund stand die Frage nach der Existenz von P-bodies in Arabidopsis thaliana und die Identifikation und Charakterisierung deren Komponenten. Weiterhin sollten Erkenntnisse über die Rolle der P-bodies unter Stressbedingungen gewonnen werden. Dabei sollten besonders Informationen über die Beziehungen zwischen den P-bodies und RNA Stressgranula (mRNA Speicherkompartimente) und Hitzestressgranula (Regulation der Proteinhomöostase) erhalten werden. Das komplette sequenzierte Genom von Arabidopsis thaliana eignete sich zur Identifikation von mRNA-Abbauproteine kodierender Gene. Unter Verwendung von Aminosäuresequenzen bereits bekannter mRNA-Abbauproteine aus Hefe und Säugerzellen konnten Homologe für die Decappingproteine Dcp1 und Dcp2 sowie für die Proteine LSm1,2,5,8 als Untereinheiten des LSm1-7 Komplexes, welcher an der Regulation der Decappingreaktion beteiligt ist, identifiziert werden. Über Hefe-Zwei-Hybrid Analysen konnten anschließend Protein-Protein-Interaktionen zwischen den untersuchten Proteinen identifiziert werden. Weiterhin konnte unter Einsatz der BIFC-Analyse gezeigt werden, dass die Interaktionen zwischen den untersuchten Proteinen hauptsächlich in zytoplasmatischen Strukturen stattfanden. Aufbauend auf diesen Befunden wurde ein Antikörper gegen Dcp1 als Marker für die zytoplasmatischen Strukturen erstellt. Dieser ermöglichte erstmals die Detektion der endogenen Strukturen in Arabidopsis thaliana. Die weitere Charakterisierung über Immunofluoreszenzanalysen zeigten, dass diese P-bodies sind. Wie die P-bodies anderer Organismen sind sie hochdynamisch und benötigen untranslatierte mRNA für die Assemblierung. Die Größe und Anzahl der P-bodies hängt dabei vom Verhältniss des Zuflusses von mRNA und der mRNA-Abbaurate ab. Weiterhin konnte beobachtet werden, das die P-bodies besonders groß unter Stressbedingungen sind und deuten eine wichtige Funktion des mRNA-Abbaus unter Stress an. Dies führte zu der Frage nach der Beziehung der P-bodies zu RNA Stressgranula, die der Speicherung von mRNA unter Stressbedingungen dienen, sowie zu Hitzestressgranula, die an der Aufrechterhaltung der Proteinhomöostase beteiligt sind. Durch Kolokalisationsanalysen mit Markern der RNA Stressgranula, der Hitzestressgranula und der P-bodies konnte erstmals gezeigt werden, dass es sich um voneinander unabhängige Mikrokompartimente handelt, und dass unter Stressbedingungen die zellulären Prozesse mRNA-Abbau, mRNA-Speicherung und Aufrechterhaltung der Proteinhomöostase auf einzelne Mikrkompartimente beschränkt sind. Allerdings konnte zwischen P-bodies und RNA Stressgranula häufig eine räumliche Nähe beobachtet werden. Dies deutet auf einen Austausch von Komponenten zwischen diesen Strukturen hin. Zusammen zeigen die erhaltenen Ergebnisse, dass die identifizierten Proteine Komponenten des 5'-3'mRNA-Abbaus darstellen, und dass der 5'-3'mRNA-Abbau in Pflanzen auch in P-bodies stattfindet. Die Identifizierung und Charakterisierung der pflanzlichen P-bodies bildet eine Grundlage für zukünftige Untersuchungen. Vor allem die massive Bildung von P-bodies unter Stressbedingungen und die Interaktion der P-bodies mit RNA Stressgranula zeigen neue Aspekte der pflanzlichen Hitzestressantwort auf.
