Thermal Models: 1) Introduction: Hadrons, Quarks, A+A 2) Statistical Mechanics of the HG (chemical potentials) 3) Hadron Matter QGP 4) Chemical Freeze-Out (hadron multiplicities) 5) Thermal Freeze-Out (hadron spectra) 6) Exact Charge Conservation: GCE CE MCE 1
u m (Me. V) d s c b t ~5 ~ 10 ~1500 ~ 5000 ~1. 7*10^5 B Baryon Number 1/3 1/3 1/3 Q Electric Charge 2/3 -1/3 2/3 S Strangeness 0 0 -1 0 0 0 C Charm 0 0 0 1 0 0 Beauty 0 0 -1 0 Top 0 0 0 1 Colour Gluon red green mg = 0 , j = 1 blue 8 charge (colour) states Straight gluon-gluon interactions 2
QCD I. Confinement II. Asymptotic Freedom I. Mesons Baryons Anti-baryons II. QGP weakly interacting gluons, quarks, anti-quarks 3
Statistical Mechanics in CE
Statistical Mechanics in GCE
MCE
MCE and CE
CE and GCE
Relativistic Statistical Mechanics in GCE
Particles i - ? Hadron Gas i: QGP i: B, Q, S 11
Hadron-Resonance Gas, GCE, Boltzmann approximation One-particle Partition function Independent variables
Baryon B and Strange S charges protons + neutrons B>0, S=0: 13
Baryon B, Strange S and Electric Q charges B>0 S=0 Q At high collision energy 14
Mean Multiplicity 15
Mean Multiplicity 16
Particle Number Distribution There are no correlations. Particle number distribution is a product of Poisson distributions GCE – no correlations Boltzmann – Poisson: scaled variance = 1
Quantum Particle in a Box One-dimensional plane wave: Periodic boundary conditions:
Quantum Ideal Gas
Quantum Ideal Gas Bosons Fermions
Number of States in
Boltzmann approximation
Fermi Distribution Non-relativistic approximation: 24
Bose Distribution Bose Condensation: decreases with T Bose Condensate 25
Bose Fermi Boltzmann
Bose Fermi Boltzmann
Bose Fermi Boltzmann
Scaled Variance Bose Fermi
Chemical potentials B, Q, S = const A A In the QGP 30
Ideal Gas Ideal Gluon Gas: Spin Colors S-B Law Ideal Gas EOS for massless particles 31
Ideal Quark-Gluon Gas anti q 16 Fermi 16+31. 5 = 47. 5 3 (u, d, s) 6 = 3 colors X 2 spin If 32