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QCD (Quantum ChromoDynamics)

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Presentation on theme: "QCD (Quantum ChromoDynamics)"— Presentation transcript:

1 QCD (Quantum ChromoDynamics)
NA60 Dilepton Data: Invariant Mass Spectra Finite Size Effects on Dilepton Properties in Relativistic Heavy Ion Collisions -QCD describes the interactions between quarks and gluons. -There are six flavors of quarks, and eight gluons, all carrying color charge Trent Strong, Texas A&M University -The force between quarks is strong and is linear in distance! (coupling constant αs≈1) -Force weakens at small distances (or high energies), so quarks essentially free within close distances (asymptotic freedom) Advisors: Dr. Ralf Rapp, Dr. Hendrik van Hees Texas A&M University Development of excess with centrality, broadening of ρ spectral shape Time Evolution of Relativistic Heavy-Ion Collision Two-Component Model Idea: Attempt to model spectra using two contributions… -Cocktail: Component from hard- scattering processes; surface contribution -Thermal or In-Medium: Components from thermal medium, such as QGP or hadron gas; bulk contribution Relativistic Heavy-Ion Collisions Collision Zone -Colliders accelerate nuclei to very relativistic speeds! (RHIC, γ ≈ 10, v=.995c) -Nuclei collide, a hot and dense region is formed -In this region, QGP and other forms of exotic matter like a hadron gas can form -They allow us to test further the theory of QCD and explore the early universe b Total Spectra = a ∙ (Thermal) + b ∙ (Cocktail) At NA60: 158 GeV/Nucleon Results: Naive Two-Component Model Electromagnetic Probes: Dileptons and Photons Peripheral Semiperipheral Quark-Gluon Plasma Dileptons and photons good sources of information from a hot and dense medium since they: a.) are produced abundantly, and throughout the history of the collision. b.) do not interact strongly with the medium. The particles carry this information via their invariant mass and 4-momentum. -Quark-Gluon Plasma (QGP)- form of matter predicted by QCD at high temperature and density. -Predicted transition temperature is ~ 170 MeV, corresponding to a temperature on the order of 1012 K. -As density and temperature become very large, hadrons formed by quarks overlap => quarks lose their affiliation with any particular hadron. -Quarks and gluons form a hot and dense soup! M [GeV] M [GeV] Semicentral Central The ρ meson is the dominant producer of dileptons. M [GeV] M [GeV] Semicentral pT < 0.5 GeV Semicentral pT > 1.0 GeV


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