Chiral phase transition and kaon-to-pion ratios in the entanglement SU(3) PNJL model

被引:7
作者
Blaschke, D. [1 ,2 ,3 ]
Friesen, A., V [1 ]
Kalinovsky, Yu L. [1 ,4 ]
Radzhabov, A. [5 ,6 ]
机构
[1] Joint Inst Nucl Res, Dubna 141980, Russia
[2] Univ Wroclaw, Inst Theoret Phys, PL-50204 Wroclaw, Poland
[3] Natl Res Nucl Univ MEPhI, Moscow 115409, Russia
[4] Dubna State Univ, Dubna 141982, Russia
[5] Matrosov Inst Syst Dynam & Control Theory, Irkutsk 664033, Russia
[6] Irkutsk State Univ, Karl Marx Str 1, Irkutsk 664003, Russia
关键词
BETH-UHLENBECK APPROACH; HADRON-PRODUCTION; FREEZE-OUT; QCD; HADRONIZATION; CONDENSATE; COLLISIONS; MATTER; NAMBU; TIME;
D O I
10.1140/epjst/e2020-000218-1
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Within the three-flavor PNJL and EPNJL chiral quark models we have obtained pseudoscalar meson properties in quark matter at finite temperature T and baryochemical potential mu(B). We compare the meson pole (Breit-Wigner) approximation with the Beth-Uhlenbeck (BU) approach that takes into account the continuum of quark-antiquark scattering states when determining the partial densities of pions and kaons. We evaluate the kaon-to-pion ratios along the (pseudo-)critical line in the T - mu(B) plane as a proxy for the chemical freezeout line, whereby the variable x = T/mu(B) is introduced that corresponds to the conserved entropy per baryon as initial condition for the heavy-ion collision experiments. We present a comparison with the experimental pattern of kaon-to-pion ratios within the BU approach and using x-dependent pion and strange quark potentials. A sharp "horn" effect in the energy dependence K+/pi(+) ratio is explained by the enhanced pion production at energies above root s(NN)=8 GeV, when the system enters the regime of meson dominance. This effect is in line with the enhancement of low-momentum pion spectra that is discussed as a precursor of the pion Bose condensation and entails the occurrence of a nonequilibrium pion chemical potential of the order of the pion mass. We elucidate that the horn effect is not related to the existence of a critical endpoint in the QCD phase diagram.
引用
收藏
页码:3517 / 3536
页数:20
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