Thermal Models 1 Introduction Hadrons Quarks AA 2

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Thermal Models: 1) Introduction: Hadrons, Quarks, A+A 2) Statistical Mechanics of the HG (chemical

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 ~

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

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 CE

Statistical Mechanics in GCE

Statistical Mechanics in GCE

MCE

MCE

MCE and CE

MCE and CE

CE and GCE

CE and GCE

Relativistic Statistical Mechanics in GCE

Relativistic Statistical Mechanics in GCE

Particles i - ? Hadron Gas i: QGP i: B, Q, S 11

Particles i - ? Hadron Gas i: QGP i: B, Q, S 11

Hadron-Resonance Gas, GCE, Boltzmann approximation One-particle Partition function Independent variables

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 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

Baryon B, Strange S and Electric Q charges B>0 S=0 Q At high collision energy 14

Mean Multiplicity 15

Mean Multiplicity 15

Mean Multiplicity 16

Mean Multiplicity 16

Particle Number Distribution There are no correlations. Particle number distribution is a product of

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 Particle in a Box One-dimensional plane wave: Periodic boundary conditions:

Quantum Ideal Gas

Quantum Ideal Gas

Quantum Ideal Gas Bosons Fermions

Quantum Ideal Gas Bosons Fermions

Number of States in

Number of States in

Boltzmann approximation

Boltzmann approximation

Fermi Distribution Non-relativistic approximation: 24

Fermi Distribution Non-relativistic approximation: 24

Bose Distribution Bose Condensation: decreases with T Bose Condensate 25

Bose Distribution Bose Condensation: decreases with T Bose Condensate 25

Bose Fermi Boltzmann

Bose Fermi Boltzmann

Bose Fermi Boltzmann

Bose Fermi Boltzmann

Bose Fermi Boltzmann

Bose Fermi Boltzmann

Scaled Variance Bose Fermi

Scaled Variance Bose Fermi

Chemical potentials B, Q, S = const A A In the QGP 30

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

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,

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

The Phase Diagramm QGP Hadrons Bag Model 33

The Phase Diagramm QGP Hadrons Bag Model 33

Energy Density QGP Mixed Phase Hadrons 34

Energy Density QGP Mixed Phase Hadrons 34

The Phase Diagramm QGP Hadron Gas 35

The Phase Diagramm QGP Hadron Gas 35

Hadron Gas Model S=0 C=0 Resonance Decays: 36

Hadron Gas Model S=0 C=0 Resonance Decays: 36