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HIGH ENERGY NUCLEAR PHYSICS (Relativistic heavy ion collisions)
wan ahmad tajuddin wan abdullah jabatan fizik universiti malaya national centre for particle physics December 2014
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And it is He who created the heavens and the earth in six days - and His Throne had been upon water - that He might test you as to which of you is best in deed. But if you say, "Indeed, you are resurrected after death," those who disbelieve will surely say, "This is not but obvious magic."
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@ LHC, CERN
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Hot dense nuclear matter
Quark-gluon plasma Hot dense nuclear matter
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CERN 17 GeV/ nucleon Pb LBL 1-2 GeV/ nucleon JINR 6 GeV/ nucleon BNL BNL 200 GeV/ nucleon pair Cu, Au, U CERN 2.76 TeV/ nucleon pair Pb
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why condition in first microseconds in hot Big Bang
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arXiv:
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Elementary particles and fields
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hadrons
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quantum chromodynamics
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why QCD state at high temperatures
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why Hadronization (~ confinement)
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regime Typical temperature range – T = 300 MeV/k = 3.3 x 1012 K
10,000 x greater than in center of Sun Corresponding energy density – e =10 GeV/ fm3 Corresponding relativistic matter pressure – P ≈ e/3 = 0.52 x 1031 bar
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Strangeness enhancement
high temperature → strangeness enhanced Statistics: particle ratios → Tch , mB at chemical freezeout Experimental: 160 MeV < Tch < 180 MeV cf. expected QCD phase transition value ~170 MeV (lattice QCD calculations)
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Heavy quarkonium suppression
hot and deconfined medium – quarkonia (cf naked flavours) expected to “melt”
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Jet quenching images courtesy CERN
coloured particles damped in coloured media
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Elliptic flow Collective anisotropy thermalization, hydrodynamics liquid-like
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Colour glass condensate
BFKL dynamics – saturation at Q2s ~ <Npart>/2 expect nch/A ~ 1/as(Q2s)
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Collective effects Ridges – final state correlations
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conclusions Quark-gluon plasma – perfect fluid
Final state correlations? Many more new and interesting things in physics related to the nucleus
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Thank you
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