![]() Elliptic flow and higher flow harmonicsħ. Basics of proton-proton and nucleus-nucleus Collisions ![]() Physics of the critical endpoint ( PBM )ģ. ![]() It is thought that shortly after the Big Bang the early universe was filled with incredibly hot quark-gluon plasma. Thermal photons and dileptons ( Schmah ) Exercise_from_09072021ġ6.07. At very high temperatures about one million times hotter than the center of the Sun quarks and gluons break free from their parent nucleons and instead form a dense, hot soup known as quark-gluon plasma. Hanbury Brown-Twiss correlations (HBT) ( PBM )Ġ9.07. Hard Scattering and nuclear modification factor ( Schmah )Įxercise_from_25062021 code Solution_25062021Ġ2.07. Space-time evolution of the QGP (flow) ( Schmah )Įxercise_from_11062021 code data Solution_11062021ġ8.06. Statistical hadronization model and charmonia/quarkonia (SHMc) ( PBM )ġ1.06. Statistical hadronization model (SHM) and strangeness ( PBM )Ġ4.06. Basics of proton-proton and nucleus-nucleus collisions ( Schmah ) Exercise codeġ4.05. Thermodynamics of the QGP (ideal gas, lattice) ( PBM ) Exercise Exercise_part2 code_part2Ġ7.05. Kinematic variables / detector overview and analysis tools ( Schmah ) Exerciseģ0.04. ![]() The QGP is a hot and densce Quantum-Chromo Dynamic (QCD) medium, created in ultrarelativisic heavy-ion collisions at the Large Hadron Collider (LHC) at CERN.Ģ3.04. The ATLAS experiment at CERN sees possible evidence of quark-gluon plasma production during collisions between photons and heavy nuclei inside the Large. In this lecture the basic concepts of Quark-Gluon Plasma (QGP) physics will be discussed. ![]()
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