“…We also observe that the K/π ratios measured in peripheral Au+Au reactions are smaller than the ones measured at the same number of participants but in central Cu+Cu collisions. This observation was also made at SPS energies and interpreted as being due to the different mean number of N+N collisions per projectile [7]. The theoretical calculations shown are made only for Au+Au collisions over the entire N part interval covered by nucleus-nucleus data.…”
Section: Resultsmentioning
confidence: 76%
“…The ratio of strange to non-strange particles measured in all A+A collisions shows an enhancement compared to the N+N reactions considered at the same energy. This enhancement depends on energy [4,5], system size [6,7], and collision geometry [8]. In this work we will concentrate on the dependence of the average transverse momenta, ratios of yields of anti-hadrons to hadrons (π − /π + , K − /K + , andp/p), and K/π ratios on the system size and geometry at mid-and forward rapidity.…”
We report on preliminary identified particle ratios from Au+Au collisions at √ s N N = 62.4 GeV in different centrality classes, measured with the BRAHMS spectrometer. Results from Cu+Cu and p+p collisions at mid-rapidity at the same energy are also included. The average transverse momenta of particle spectra, antiparticle to particle ratios and K/π ratios dependence on centrality and rapidity are shown and discussed.
“…We also observe that the K/π ratios measured in peripheral Au+Au reactions are smaller than the ones measured at the same number of participants but in central Cu+Cu collisions. This observation was also made at SPS energies and interpreted as being due to the different mean number of N+N collisions per projectile [7]. The theoretical calculations shown are made only for Au+Au collisions over the entire N part interval covered by nucleus-nucleus data.…”
Section: Resultsmentioning
confidence: 76%
“…The ratio of strange to non-strange particles measured in all A+A collisions shows an enhancement compared to the N+N reactions considered at the same energy. This enhancement depends on energy [4,5], system size [6,7], and collision geometry [8]. In this work we will concentrate on the dependence of the average transverse momenta, ratios of yields of anti-hadrons to hadrons (π − /π + , K − /K + , andp/p), and K/π ratios on the system size and geometry at mid-and forward rapidity.…”
We report on preliminary identified particle ratios from Au+Au collisions at √ s N N = 62.4 GeV in different centrality classes, measured with the BRAHMS spectrometer. Results from Cu+Cu and p+p collisions at mid-rapidity at the same energy are also included. The average transverse momenta of particle spectra, antiparticle to particle ratios and K/π ratios dependence on centrality and rapidity are shown and discussed.
“…2 that the thermal model delivers for pp andpp collisions [ 11] values of γ s compatible with peripheral collisions. [ 12,13] and central C+C and Si+Si data [ 9] under various fit conditions, assuming 50% feeding from weak decays. Also shown is the fraction of participants which underwent multiple collisions, f 2 .…”
The dependence of the strangeness saturation factor on the system size,
centrality and energy is studied in relativistic heavy-ion collisions.Comment: contribution for Proc. 19th Winter Workshop on Nuclear Dynamics,
Breckenridge, February 8-15, 200
“…Within the past years, physicists aimed at revealing the very nature of strongly interacting matter experimentally by ultra-relativistic heavy-ion collisions performed at CERN-SPS and BNL-RHIC (see e. g. [1,2]). At the large local energy densities reached during the collision process, a new state of deconfined matter, dubbed quark-gluon plasma (QGP), is thought to be created.…”
Within a phenomenological quasiparticle model, the quark mass and temperature dependence of the QCD equation of state is discussed and compared with lattice QCD results. Different approximations for the quasiparticle dispersion relations are employed, scaling properties of the equation of state with quark mass and deconfinement temperature are investigated and a continuation to asymptotically large temperatures is presented.
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