Diagonal and off-diagonal susceptibilities of conserved quantities in relativistic heavy-ion collisions
arXiv:1606.09573 · doi:10.1088/0954-3899/43/12/125103
Abstract
Susceptibilities of conserved quantities, such as baryon number, strangeness and electric charge are sensitive to the onset of quantum chromodynamics (QCD) phase transition and are expected to provide information on the matter produced in heavy-ion collision experiments. A comprehensive study of the second-order diagonal susceptibilities and cross correlations has been made within a thermal model approach of the hadron resonance gas (HRG) model as well as with a hadronic transport model, UrQMD. We perform a detailed analysis of the effect of detector acceptances and choice of particle species in the experimental measurements of the susceptibilities for heavy-ion collisions corresponding to \sNN = 4 GeV to 200 GeV. The transverse momentum cutoff dependence of suitably normalised susceptibilities are proposed as useful observables to probe the properties of the medium at freezeout.
16 pages, 11 figures
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Cited by in corpus (21)
- Theoretical and Experimental Constraints for the Equation of State of Dense and Hot Matter
- Off-diagonal correlators of conserved charges from lattice QCD and how to relate them to experiment
- Collision energy dependence of second-order off-diagonal and diagonal cumulants of net-charge, net-proton and net-kaon multiplicity distributions in Au+Au collisions
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- Rapidity dependence of proton cumulants and correlation functions
- Freezeout systematics due to the hadron spectrum
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- Baryon-Strangeness Correlations in Au+Au Collisions at =7.7-200 GeV from the UrQMD model
- Multiplicity and pseudorapidity density distributions of charged particles produced in pp, pA and AA collisions at RHIC \& LHC energies
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- Effects of centrality fluctuation and deuteron formation on proton number cumulant in Au+Au collisions at = 3 GeV from JAM model
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- Effect of Coriolis Force on Diffusion of D Meson
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- Shear viscosity and electrical conductivity of rotating quark matter in Nambu--Jona-Lasinio Model
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