Thermal hadron production in high energy collisions
arXiv:hep-ph/9708248 · doi:10.1088/0954-3899/23/12/017
Abstract
It is shown that hadron abundances in high energy e+e-, pp and p{\bar p} collisions, calculated by assuming that particles originate in hadron gas fireballs at thermal and partial chemical equilibrium, are in very good agreement with the data. The freeze-out temperature of the hadron gas fireballs turns out to be nearly constant over a large center of mass energy range and not dependent on the initial colliding system. The only deviation from chemical equilibrium resides in the incomplete strangeness phase space saturation. Preliminary results of an analysis of hadron abundances in S+S and S+Ag heavy ion collisions are presented.
10 pages, 1 .eps figure, talk given at the Strangeness and Quark Matter 97 conference
References in corpus (1)
Cited by in corpus (39)
- Relativistic Hadron-Hadron Collisions in the Ultra-Relativistic Quantum Molecular Dynamics Model (UrQMD)
- THERMINATOR 2: THERMal heavy IoN generATOR 2
- Therminator: Thermal heavy-Ion generator
- Statistical Coalescence Model with Exact Charm Conservation
- Open Heavy-Flavor Production in Heavy-Ion Collisions
- The Thermal Production of Strange and Non-Strange Hadrons in e+e- Collisions
- D meson production at central rapidity in proton-proton collisions at = 7 TeV
- Centrality dependence of hadronization and chemical freeze-out conditions in heavy ion collisions at \sqrt s_{NN} = 2.76 TeV
- Cascade and anti-cascade production in central Pb+Pb collisions at 158 GeV/c per nucleon
- Bose-Einstein condensation of pions in heavy-ion collisions at the CERN Large Hadron Collider (LHC) energies
- Explanation of hadron transverse-momentum spectra in heavy-ion collisions at sqrt(sNN) = 2.76 TeV within chemical non-equilibrium statistical hadronization model
- Thermal description of hadron production in e+e- collisions revisited
- Statistical hadronization of heavy flavor quarks in elementary collisions: successes and failures
- Chemical equilibration of strangeness
- Particle production in p-p collisions and prediction for LHC energy
- Towards the Quark-Gluon Plasma
- Universal pion freeze-out phase-space density
- Transverse-momentum spectra of strange particles produced in Pb+Pb collisions at TeV in the chemical non-equilibrium model
- Quark model and strange baryon production in heavy ion collisions
- Open Charm Enhancement in Pb+Pb Collisions at SPS
- Signals of the quark-gluon plasma in nucleus-nucleus collisions
- Heavy baryonic resonances, multistrange hadrons, and equilibration at energies available at the GSI Schwerionensynchrotron, SIS18
- Heavy quark(onium) at LHC: the statistical hadronization case
- Single-freeze-out model for ultra relativistic heavy-ion collisions at TeV and the LHC proton puzzle
- Probing the boundaries of the Hadronic Phase through a Strangeness including Statistical Bootstrap Model (S-SBM)
- Canonical Statistical Model and hadron production in annihilations
- Constrains for non-standard statistical models of particle creations by identified hadron multiplicity results at LHC energies
- Hadron production from resonance decay in relativistic collisions
- Particle production in p-p collisions at sqrt(s) = 17 GeV within the statistical model
- Entropy and Heat Capacity of the transverse momentum distribution for pp collisions at RHIC and LHC energies
- Time Dependence of Chemical Freeze-out in Relativistic Heavy Ion Collisions
- A statistical method to estimate low-energy hadronic cross sections
- Locally anisotropic momentum distributions of hadrons at freeze-out in relativistic heavy-ion collisions
- Sigma-antihyperon correlations in Z0 decay and investigation of the baryon production mechanism
- Study of strange particle production in pp collisions with the ALICE detector
- Universal Pion Freeze-out Phase-Space Density
- Is Strangeness still interesting at RHIC ?
- The strange-quark chemical potential as an experimentally accessible "order parameter" of the deconfinement phase transition for finite baryon-density
- Thermal nature of confining strings