Dirk H. Rischke

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Quarks O. Scavenius, Á. Mócsy, I.N. Mishustin and D.H. Rischke 1The Niels Bohr Institute, Blegdamsvej 17 DK–2100 Copenhagen Ø, Denmark 2School of Physics and Astronomy, University of Minnesota Minneapolis, MN 55455, USA 3The Kurchatov Institute, Russian Research Center Moscow 123182, Russia 4Institut für Theoretische Physik, J. W. Goethe Unerversität,(More)
1 Physics Dept., Duke Univ., Durham, NC, USA, 2 Inst. Theor. Phys., J.W. Goethe Univ., Frankfurt am Main, Germany, 3 Inst. Theor. Phys., Univ. Giessen, Germany, 4 Physics Dept., Yale Univ., New Haven, CT, USA, 5 Subatech, Univ. Nantes, France, 6 Jyvaskyla Univ., Finland, 7 Phys. Dept., Columbia Univ., New York, NY, USA, 8 Phys. Dept. and RBRC, Brookhaven(More)
We solve the relativistic Riemann problem in viscous gluon matter employing a microscopic parton cascade. We demonstrate the transition from ideal to viscous shock waves by varying the shear viscosity to entropy density ratio eta/s from zero to infinity. We show that an eta/s ratio larger than 0.2 prevents the development of well-defined shock waves on time(More)
We discuss QCD with two light flavors at large baryon chemical potential micro. Color superconductivity leads to partial breaking of the color SU(3) group. We show that the infrared physics is governed by the gluodynamics of the remaining SU(2) group with an exponentially soft confinement scale Lambda(')(QCD) approximately Deltaexp[-a(mu)/(gDelta)], where(More)
Collisions of elementary particles, hadrons, and nuclei at ultrarelativistic energies produce a multitude of particles (“multiparticle production”). Final-state interactions between the produced particles determine the dynamical evolution of the system. In ee and hadron-hadron collisions only few particles are produced, and it is unlikely that many(More)
The classical Yang–Mills equations are solved perturbatively in covariant gauge for a collision of two ultrarelativistic nuclei. The nuclei are taken as ensembles of classical color charges on eikonal trajectories. The classical gluon field is computed in coordinate space up to cubic order in the coupling constant g. We construct the Feynman diagrams(More)