795 research outputs found
Thermal hadron production in pp and p{\bar p} collisions
It is shown that the hadron production in high energy pp and p{\bar p}
collisions, calculated by assuming that particles originate in hadron gas
fireballs at thermal and partial chemical equilibrium, agrees very well with
the data. The temperature of the hadron gas fireballs, determined by fitting
hadron abundances, does not seem to depend on the centre of mass energy, having
a nearly constant value of about 170 MeV. This value is in agreement with that
obtained in e^+e^- collisions and supports a universal hadronization mechanism
in all kinds of reactions consisting in a parton-hadron transition at critical
values of temperature and pressure.Comment: 41 pages, 11 .eps figures, published in Z. Phys. C Revision -
Corrections of two formulae in Sect.
What is the meaning of the statistical hadronization model?
The statistical model of hadronization succeeds in reproducing particle
abundances and transverse momentum spectra in high energy collisions of
elementary particles as well as of heavy ions. Despite its apparent success,
the interpretation of these results is controversial and the validity of the
approach very often questioned. In this paper, we would like to summarize the
whole issue by first outlining a basic formulation of the model and then
comment on the main criticisms and different kinds of interpretations, with
special emphasis on the so-called "phase space dominance". While the ultimate
answer to the question why the statistical model works should certainly be
pursued, we stress that it is a priority to confirm or disprove the fundamental
scheme of the statistical model by performing some detailed tests on the rates
of exclusive channels at lower energy.Comment: 14 pages, to be published in the Proceedings of the International
workshop "Focus on multiplicity", Bari (Italy) June 17-19 200
Universal Pion Freeze-out Phase-Space Density
Results on the pion freeze-out phase-space density in sulphur-nucleus, Pb-Pb
and pion-proton collisions at CERN-SPS are presented. All heavy-ion reactions
are consistent with the thermal Bose-Einstein distrtibution f=1/(exp(E/T)-1) at
T~120 MeV, modified for expansion. Pion-proton data are also consistent with f,
but at T~180 MeV.Comment: 1 page, 1 figure; 98' report for GSI-Darmstad
Strange quark production in a statistical effective model
An effective model with constituent quarks as fundamental degrees of freedom
is used to predict the relative strangeness production pattern in both high
energy elementary and heavy ion collisions. The basic picture is that of the
statistical hadronization model, with hadronizing color-singlet clusters
assumed to be at full chemical equilibrium at constituent quark level. Thus, by
assuming that at least the ratio between strange and non-strange constituent
quarks survives in the final hadrons, the apparent undersaturation of strange
particle phase space observed in the data can be accounted for. In this
framework, the enhancement of relative strangeness production in heavy ion
collisions in comparison with elementary collisions is mainly owing to the
excess of initial non-strange matter over antimatter and the so-called
canonical suppression, namely the constraint of exact color and flavor
conservation over small volumes.Comment: 22 pages, 9 postscript figures, slightly shortened version published
in Phys. Rev.
Statistical hadronization with exclusive channels in e+e- annihilation
We perform a systematic analysis of exclusive hadronic channels in e+e-
collisions at centre-of-mass energies between 2.1 and 2.6 GeV within the
statistical hadronization model. Because of the low multiplicities involved,
calculations have been carried out in the full microcanonical ensemble,
including conservation of energy-momentum, angular momentum, parity, isospin,
and all relevant charges. We show that the data is in an overall good agreement
with the model for an energy density of about 0.5 GeV/fm^3 and an extra
strangeness suppression parameter gamma_S ~ 0.7, essentially the same values
found with fits to inclusive multiplicities at higher energy.Comment: 27 pages, 12 figure
Antihyperon-Production in Relativistic Heavy Ion Collision
Recently it has been shown that the observed antiproton yield in heavy-ion
collisions at CERN-SpS energies can be understood by multi-pionic interactions
which enforce local chemical equilibrium of the antiprotons with the nucleons
and pions. Here we show that antihyperons are driven towards local chemical
equilibrium with pions, nucleons and kaons on a timescale of less than 3 fm/c
when applying a similar argument for the antihyperons by considering the
inverse channel of annihilation reactions anti-Y + p to pions + kaons. These
multi-mesonic reactions easily explain the antihyperon yields at CERN-SpS
energies as advertised in pure thermal, hadronic models without the need of a
quark gluon plasma phase. In addition, the argument also applies for AGS
energies.Comment: 4 pages using RevTeX, 1 eps figur
Fluctuations of particle ratios and the abundance of hadronic resonances
In this letter we will argue that the event-by-event fluctuations of the
ratio of positively over negatively charged pions provides a measurements of
the number of rho and omega mesons right after hadronization. This finding can
be utilized to put the hypothesis of chemical equilibration in relativistic
heavy ion collisions to a test.Comment: 4 pages. No figure. Uses revtex with prl, aps, and multicol style
Status of Chemical Equilibrium in Relativistic Heavy Ion Collisions
Recent work on chemical equilibrium in heavy ion collisions is reviewed. The
energy dependence of thermal parameters is discussed. The centrality dependence
of thermal parameters at SPS energies is presented.Comment: 7 pages, 7 Postscript figure
Overpopulation of in pp collisions: a way to distinguish statistical hadronization from string dynamics
The ratio originating from string decays is predicted
to be larger than unity in proton proton interactions at SPS energies (=160 GeV). The anti-omega dominance increases with decreasing beam energy.
This surprising behavior is caused by the combinatorics of quark-antiquark
production in small and low-mass strings. Since this behavior is not found in a
statistical description of hadron production in proton proton collisions, it
may serve as a key observable to probe the hadronization mechanism in such
collisions.Comment: 4 pages, 4 figure
Is Strangeness still interesting at RHIC ?
With the advent of the Relativistic Heavy Ion Collider (RHIC) at Brookhaven
National Laboratory (BNL), Heavy Ion Physics will enter a new energy regime.
The question is whether the signatures proposed for the discovery of a phase
transition from hadronic matter to a Quark Gluon Plasma (QGP), that were
established on the basis of collisions at the BEVALAC, the AGS, and the SPS,
respectively, are still useful and detectable at these high incident energies.
In the past two decades, measurements related to strangeness formation in the
collision were advocated as potential signatures and were tested in numerous
fixed target experiments at the AGS and the SPS. In this article I will review
the capabilities of the RHIC detectors to measure various aspects of
strangeness, and I will try to answer the question whether the information
content of those measurements is comparable to the one at lower energies.Comment: 12 pages, 7 figures, Invited Talk at the IV International Conference
on Strangeness in Quark Matter, Padova (Italy), July 20-24, 199
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