2000
DOI: 10.1146/annurev.nucl.50.1.299
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Strangeness Production in Heavy-Ion Collisions

Abstract: ▪ Abstract  Strangeness production is a very useful diagnostic tool in finding the quark-gluon plasma. We review its uses in understanding relativistic heavy-ion collisions. A brief introduction to the main theoretical tools used in interpreting strangeness production is given, and the experimental methods used to extract the signals are discussed in detail. The experimental results from the Brookhaven AGS and CERN SPS programs are presented. We discuss the interpretation of these results, emphasizing their ro… Show more

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Cited by 29 publications
(18 citation statements)
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“…The temperature parameter is found in all high energy collisions (pp, e + e − , A+A) to be about 160 -170 MeV, while γ s increases from 0.5 − 0.6 in pp to 0.9 − 1 in A+A [61,62]. The disappearance of strangeness suppression in nuclear collisions [63,64], usually called strangeness enhancement, was one of the first signals predicted for the QGP [65], and the fact that the bulk of all particles are produced in heavy ion reactions with thermal ratios to very good approximation (typically < 10-20%) is considered to be an essential and well established fact. Fig.…”
Section: Identified Particle Yieldsmentioning
confidence: 99%
“…The temperature parameter is found in all high energy collisions (pp, e + e − , A+A) to be about 160 -170 MeV, while γ s increases from 0.5 − 0.6 in pp to 0.9 − 1 in A+A [61,62]. The disappearance of strangeness suppression in nuclear collisions [63,64], usually called strangeness enhancement, was one of the first signals predicted for the QGP [65], and the fact that the bulk of all particles are produced in heavy ion reactions with thermal ratios to very good approximation (typically < 10-20%) is considered to be an essential and well established fact. Fig.…”
Section: Identified Particle Yieldsmentioning
confidence: 99%
“…The temperature parameter is found in all high energy collisions (pp, e + e − , A+A) to be about 160 -170 MeV, while γ s increases from 0.5 − 0.6 in pp to 0.9 − 1 in A+A [12,23]. This disappearance of strangeness suppression in nuclear collisions [24,25], the so-called strangeness enhancement, and the fact that the bulk of all particles are produced in heavy-ion reactions with thermal ratios to very good approximation (typically < 10-20%) is considered to be an essential and well established fact.…”
Section: Strangeness Enhancementmentioning
confidence: 99%
“…With the availability of Pb beams at the SPS these studies were extended in the years after 1994 toward a systematic study of the system size dependence of this effect, including the rare Ω hyperon [111,112,113]. A review of the experimental results available after the first round of CERN experiments with Pb beams at 158A GeV can be found in [114]. Figure 6 shows the strange particle enhancement in Pb+Pb collisions relative to p+Be interactions as observed by the NA57 experiment [112].…”
Section: Basic Observationsmentioning
confidence: 99%
“…This method is complementary to dE/dx or TOF measurement and can provide an independent way of particle identification with different systematic effects [130]. However, there are substantial sources of background, like charged hyperon and pion decays, as well as multiple scattering in the detector material [114]. The method is limited to particles that decay inside the sensitive area of the tracking devices which reduces the available statistics.…”
Section: Charged Kaonsmentioning
confidence: 99%