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Alt, C.; Grebieszkow, K.; Yoo, I.-K.; Peryt, W.; Gładysz, E.; Eckardt, V.; Lungwitz, B.; Fodor, Z.; Schmitz, N.; Sziklai, J.; Bartke, J.; Chung, P.; Kadija, K.; Friese, V.; Siklér, F.; Csató, P.; Utvić, Milan; Słodkowski, M.; Włodarczyk, Z.; Vassiliou, M.; Białkowska, H.; Strabel, C.; László, Á.; Melkumov, G. L.; Kolesnikov, V.; Rybczyński, M.; Blume, C.; Cramer, J. G.; Panagiotou, A.; Pluta, J.; Szuba, M.; Stefanek, G.; Barna, D.; Leeuwen, M. van; Vranić, D.; Richard, A.; Kraus, I.; Chvála, O.; Roland, G.; Höhne, C.; Gál, János; Hegyi, S.; Makariev, M.; Mischke, A.; Petridis, A.; Pálla, G.; Botje, M.; Mitrovski, M.; Mrówczyński, S.; Foka, P.; Dinkelaker, P.; Baatar, B.; Kowalski, M.; Kniege, S.; Christakoglou, P.; Litov, L.; Bramm, R.; Lévai, P.; Skrzypczak, E.; Gaździcki, M.; Kornaš, E.; Sitár, B.; Šuša, T.; Antičić, T.; Flierl, D.; Lacey, R.; Rybicki, A.; Betev, L.; Ströbele, H.; Pikna, M.; Genchev, V.; Molnár, J.; Szentpétery, I.; Mateev, M.; Pühlhofer, F.; Szymański, P.; Malakhov, A.; Trubnikov, V.; Kreps, M.; Renfordt, R.; Zimànýi, J.; Prindle, D.; Bunčić, P.; Schuster, T.; Černý, V.; Karev, A.; Boimska, B.; Kliemant, M.; Kikoła, D. P.; Varga, D.; Wojtaszek, A.; Seyboth, P.; Stock, R.; Nicolic, V.; Meurer, C.; Veres, G. I.; Vesztergombi, G.; Braciník, J.; Panayotov, D.; Sandoval, A.; Wetzler, A.; Roland, C.

doi:10.1103/physrevc.78.034918

Cited by 116 publications

(36 citation statements)

References 63 publications

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“…From this figure it is also seen that lighter mesons like π − and K − show a fair agreement between experimental data [9,[13][14][15][16][17][18][19][20][21][22][23] and UrQMD prediction at all energies. However, for heavier meson like φ, as the energy of collision increases, there is a considerable disagreement between the observed and UrQMD predicted values.…”

Section: Results For Width Of Rapidity Distributionsupporting

confidence: 82%

“…In Fig. 1, the rapidity distributions of a few hadrons such as π − , k − , φ, and produced in UrQMD generated Au + Au collisions at 10, 20, 30 and 40 A GeV are plotted and compared with the existing Super Proton Synchrotron (SPS) [9,[13][14][15][16] and Alternating Gradient Synchrotron (AGS) (E802, E877, E896, E917) [17][18][19][20][21][22][23] data at the same energies. It is seen from this figure that, with UrQMD generated events, the rapidity distribution of ( + 0 ) and not alone gives a better agreement with the experimental data on .…”

Section: Results For Width Of Rapidity Distributionmentioning

confidence: 99%

“…(Color online) Variation of width of the rapidity distribution (calculated from data[9,[13][14][15][16][17][18][19][20][21][22][23]) of (a) mesons and (b) baryons as a function of beam rapidity in the laboratory system. (c) The same has been plotted separately for and φ.…”

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confidence: 99%

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Separate mass scaling of the widths of the rapidity distributions for mesons and baryons at energies available at the Facility for Antiproton and Ion Research

Dey

Bhattacharjee

2014

Phys. Rev. C

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Evolution of the width of the rapidity distribution on beam rapidity has been studied for a number of produced particles with UrQMD-3.3p1 generated events at various FAIR (Facility for Antiproton and Ion Research) energies. The results for the width of the rapidity distribution with beam rapidity, obtained with UrQMD generated events, are compared with the existing experimental data (E802, E877, E896, E917, NA49). For both UrQMD and experimental data, the width of the rapidity distribution is found to bear scaling behavior with beam rapidity for all the hadrons. Such scaling behavior is found to follow separate mass ordering for the studied mesons and and baryons.

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Section: Results For Width Of Rapidity Distributionsupporting

confidence: 82%

Section: Results For Width Of Rapidity Distributionmentioning

confidence: 99%

See 1 more Smart Citation

Separate mass scaling of the widths of the rapidity distributions for mesons and baryons at energies available at the Facility for Antiproton and Ion Research

Dey

Bhattacharjee

2014

Phys. Rev. C

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“…Strange quarks are expected to be abundant in a deconfined medium due to the short time needed to reach equilibrium values among the parton species and to the lower energy threshold for ss production. A pattern of strangeness enhancement increasing with the hadron strangeness content when going from pp (p-A) to heavy-ion collisions was observed at the SPS [31][32][33][34], at RHIC [35] and at the LHC [36]. In the frame of the statistical hadronisation models, strange particle production in heavy-ion collisions follows the expectation for a grand-canonical ensemble.…”

Section: Jhep03(2016)082mentioning

confidence: 81%

Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N = 2.76 $$ \sqrt{{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV

Adam¹,

Adamová²,

Aggarwal³

et al. 2016

J. High Energ. Phys.

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The production of prompt D + s mesons was measured for the first time in collisions of heavy nuclei with the ALICE detector at the LHC. The analysis was performed on a data sample of Pb-Pb collisions at a centre-of-mass energy per nucleon pair, √ s NN , of 2.76 TeV in two different centrality classes, namely 0-10% and 20-50%. D + s mesons and their antiparticles were reconstructed at mid-rapidity from their hadronic decay channel D + s → φπ + , with φ → K − K + , in the transverse momentum intervals 4 < p T < 12 GeV/c and 6 < p T < 12 GeV/c for the 0-10% and 20-50% centrality classes, respectively. The nuclear modification factor R AA was computed by comparing the p T -differential production yields in Pb-Pb collisions to those in proton-proton (pp) collisions at the same energy. This pp reference was obtained using the cross section measured at

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“…The (Color online) Energy dependence of the ratios K + /π + , /π + , and /p in the HRG model at midrapidity as compared to experimental data at AGS [37], SPS [38], RHIC [29,31], and LHC [34,35]. monotonous increase of antinuclei abundance with √ s NN clearly suggests that at RHIC and LHC energies reconstruction of more massive antinuclei may become feasible.…”

Section: Resultsmentioning

confidence: 99%

Production of antinuclei and hypernuclei in a relativistic Hagedorn resonance gas model

Pal

Greiner

2013

Phys. Rev. C

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Energy dependence of Λ and Ξ production in centralPb+Pbcollisions at20A,30A,40A,

Cited by 116 publications

References 63 publications

Separate mass scaling of the widths of the rapidity distributions for mesons and baryons at energies available at the Facility for Antiproton and Ion Research

Separate mass scaling of the widths of the rapidity distributions for mesons and baryons at energies available at the Facility for Antiproton and Ion Research

Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N = 2.76 $$ \sqrt{{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV

Production of antinuclei and hypernuclei in a relativistic Hagedorn resonance gas model

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