Finite Size Effects on Dilepton Properties in Relativistic Heavy Ion Collisions Trent Strong, Texas...
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![Page 1: Finite Size Effects on Dilepton Properties in Relativistic Heavy Ion Collisions Trent Strong, Texas A&M University Advisors: Dr. Ralf Rapp, Dr. Hendrik.](https://reader030.fdocuments.net/reader030/viewer/2022032523/56649d7f5503460f94a632a3/html5/thumbnails/1.jpg)
Finite Size Effects on Dilepton Properties in Relativistic Heavy Ion Collisions
Trent Strong, Texas A&M University
Advisors: Dr. Ralf Rapp, Dr. Hendrik van Hees Texas A&M University Cyclotron Institute
Cyclotron Institute REU 2006
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QCD (Quantum ChromoDynamics)
-QCD describes the interactions between quarks and gluons.
-There are six flavors of quarks, and eight gluons, all carrying color charge
-The force between quarks is strong and is linear in distance! (coupling constant α
s≈1)
-Force weakens at small distances (or high energies), so quarks essentially free within bounds (asymptotic freedom)
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Relativistic Heavy-Ion Collisions
At NA60: In-In @ 158 GeV/Nucleon
b
-Colliders accelerate nuclei to very relativistic speeds! (RHIC, γ ≈ 100, v=.9995c)
-Nuclei collide, a hot and dense region is formed
-In this region, the Quark-gluon plasma (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
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-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 particularhadron.
-Quarks and gluons form a hot and dense soup!
Quark-Gluon Plasma
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Time Evolution of Relativistic Heavy-Ion Collision
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Electromagnetic Probes: Dileptons and Photons
Dileptons and photons good sources of information from a hot and dense medium since they: a.) are produced 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.
In a hadronic medium expected from such a collision, the ρ meson is the dominant producer of dileptons.
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NA60: Dilepton DataInvariant Mass Spectra
Plots: S. Damjanovic, QM05
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NA60: Dilepton Data Transverse Momentum Spectra
-Data show signs of a two-component spectrum, one component dominates at low pT while the other dominates at high pT
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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
Collision Zone
Total Spectra = a ∙ (Thermal) + b ∙ (Cocktail)
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Results: Naive Two-Component Model in 4 Centrality Bins
M[GeV]M[GeV]
Peripheral Semiperipheral
Semicentral Central
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Naive Two-Component Model:Semicentral in two pT slices
M[GeV]
M[GeV]
pT < 0.5 GeV
pT > 1.0 GeV
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Early Conclusions
-Two Component Model seems to work well for inclusive pT bins, but shows deficiency in semicentral high-pT region.
-Need to include smaller effects, other contributions to make model more complete
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Backup Slides
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Dilepton Spectra: Theory
D
g
mTqf
Mqxdd
Nd B Im),(1
~2
4
044
8
ρ Spectral Function:
-Spectral function gives distribution of rho mesons being produced per unit four position and unit four momentum
-To obtain observed spectra, convolute over the entire spacetime history of the fireball expansion.