Baryon Rapidity Loss in Relativistic<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>A</mml:mi><mml:mi>u</mml:mi><mml:mo>+</mml:mo><mml:mi>A</mml:mi><mml:mi>u</mml:mi></mml:math>Collisions

Back, B. B.; Betts, R. R.; Chang, James; Chang, W. C.; Y., C.; Chu, Y. Y.; Cumming, J. B.; Dunlop, J. C.; Eldredge, W.; Fung, S. Y.; Ganz, R.; Garcia, E. Oliver; Gillitzer, A.; Heintzelman, G.; Henning, W.; Hofman, D. J.; Holzman, B.; Kang, Joon Ho; Kim, E. J.; Kim, S. Y.; Kwon, Y.-J.; McLeod, D.; Mignerey, A. C.; Moulson, M.; Nanal, V.; Ogilvie, C. A.; Pak, R.; Ruangma, A.; Russ, D.; Seto, R.; Stanskas, P. J.; Stephans, G. S. F.; Wang, H. Q.; Wolfs, F. L. H.; Wuosmaa, A. H.; Xiang, H.; Xu, G.; Yao, H.; Zou, C.

doi:10.1103/physrevlett.86.1970

Cited by 112 publications

(47 citation statements)

References 13 publications

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“…However, for the beam energies 2, 4, 6 and 8 AGeV only a few data points are available. They corresponds to the yields for pions [16,17], for protons [18,19], for kaons [17] (except for 2 AGeV). The integrated over 4 data are also available for Λ hyperons [20] and for Ξ − hyperons (for 6 AGeV only) [22].…”

Section: Fitting Proceduresmentioning

confidence: 99%

Separate Chemical Freeze-Outs of Strange and Non-Strange Hadrons and Problem of Residual Chemical Non-Equilibrium of Strangeness in Relativistic Heavy Ion Collisions

et al. 2016

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We present an elaborate version of the hadron resonance gas model with the combined treatment of separate chemical freeze-outs for strange and non-strange hadrons and with an additional factor which accounts for the remaining strange particle non-equilibration. Within suggested approach the parameters of two chemical freezeouts are connected by the conservation laws of entropy, baryonic charge, third isospin projection and strangeness. The developed model enables us to perform a high-quality fit of the hadron multiplicity ratios measured at AGS, SPS and RHIC with 2 / ≃ 0.93. A special attention is paid to a successful description of the Strangeness Horn. The well-known problem of selective suppression ofΛ andΞ hyperons is also discussed. The main result is that for all collision energies the factor is about 1 within the error bars, except for the center of mass collision energy 7.6 GeV at which we find about 20% enhancement of strangeness. Also we confirm an existence of strong jumps in pressure, temperature and effective number of degrees of freedom at the stage of strange particle chemical freeze-out, when the center of mass collision energy changes from 4.3 to 4.9 GeV. We argue that these irregularities may signal about the quark-hadron phase transition.

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Section: Fitting Proceduresmentioning

confidence: 99%

Separate Chemical Freeze-Outs of Strange and Non-Strange Hadrons and Problem of Residual Chemical Non-Equilibrium of Strangeness in Relativistic Heavy Ion Collisions

et al. 2016

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“…Data Analysis: − We have used AGS [57][58][59][60][61][62][63][64][65], SPS [66][67][68][69][70][71][72][73][74][75], RHIC [76][77][78][79][80][81][82][83][84][85][86][87][88][89][90][91] and LHC [92][93][94][95] data for our analysis. STAR BES data has been used following [49,96,97].…”

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confidence: 99%

Novel scheme for parametrizing the chemical freeze-out surface in heavy ion collision experiments

et al. 2019

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“…We have used AGS [62][63][64][65][66][67][68][69][70], SPS [71][72][73][74][75][76][77][78][79][80], RHIC [81][82][83][84][85][86][87][88][89][90][91][92][93][94][95][96] and LHC [97][98][99][100] data for our analysis. The data for STAR BES is obtained from Ref [48,55,101].…”

Section: Discussionmentioning

confidence: 99%

Systematics of chemical freeze-out parameters in heavy-ion collision experiments

et al. 2020

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We discuss systematic uncertainties in the chemical freeze-out parameters from the χ 2 analysis of hadron multiplicity ratios in the heavy-ion collision experiments. The systematics due to the choice of specific hadron ratios are found to lie within the experimental uncertainties. The variations obtained by removing the usual constraints on the conserved charges show similar behavior. The net charge to net baryon ratios in such unconstrained systems are commensurate with the expected value obtained from the protons and neutrons of the colliding nuclei up to the center of mass energies ∼ 40 GeV. Beyond that the uncertainties in this ratio gradually increases, possibly indicating the reduction in baryon stopping.

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Baryon Rapidity Loss in RelativisticAu+AuCollisions

Cited by 112 publications

References 13 publications

Separate Chemical Freeze-Outs of Strange and Non-Strange Hadrons and Problem of Residual Chemical Non-Equilibrium of Strangeness in Relativistic Heavy Ion Collisions

Separate Chemical Freeze-Outs of Strange and Non-Strange Hadrons and Problem of Residual Chemical Non-Equilibrium of Strangeness in Relativistic Heavy Ion Collisions

Novel scheme for parametrizing the chemical freeze-out surface in heavy ion collision experiments

Systematics of chemical freeze-out parameters in heavy-ion collision experiments

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