DYNAMICAL MODELING OF RELATIVISTIC HEAVY- ION COLLISIONS AT BEAM ENERGY SCAN ENERGIES CHUN SHEN RBRC RIKEN BNL Research Center UH/UIUC Journal Club Oct. 16, 2020

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 2 Initial energy density Hadronization Kinetic freeze-out final detected particles distributions QGP phase e+ e- Hadron gas phase τ ~ 0 fm/c τ ~ 1 fm/c pre- equilibrium dynamics Relativistic Heavy-Ion Collisions free streaming τ ~ 10 fm/c viscous hydrodynamics collision evolution π K p τ ~ 1015 fm/c Complex dynamics driven by multiple length scales Hybrid multi-stage modeling with event-by-event fluctuations RELATIVISTIC HEAVY-ION COLLISIONS

Chun Shen (WSU/RBRC) UH/UIUC Journal Club DEFINING THE QUARK-GLUON PLASMA Which properties of hot QCD matter can we determine from relativistic heavy ion data (LHC, RHIC, and future FAIR/NICA/JPAC)? Electromagnetic emissivity Equation of State DB, DQ, DS AAAB+nicdVDLSgMxFM3UV62vqS7dBIvgogwzVdTuSu3CZYv2Ae0wZNJMG5rJDElGKWM/xY0LRdz6Je78G9OH4PPA5R7OuZfcHD9mVCrbfjcyS8srq2vZ9dzG5tb2jpnfbckoEZg0ccQi0fGRJIxy0lRUMdKJBUGhz0jbH11M/fYNEZJG/FqNY+KGaMBpQDFSWvLMfM2rFntFWPMa83blmQXbKttO+dSBv4lj2TMUwAJ1z3zr9SOchIQrzJCUXceOlZsioShmZJLrJZLECI/QgHQ15Sgk0k1np0/goVb6MIiELq7gTP26kaJQynHo68kQqaH86U3Fv7xuooJzN6U8ThTheP5QkDCoIjjNAfapIFixsSYIC6pvhXiIBMJKp5XTIXz+FP5PWiXLObZKjZNCpbqIIwv2wQE4Ag44AxVwCeqgCTC4BffgETwZd8aD8Wy8zEczxmJnD3yD8foBUi+SHg== Charge diffusion Spectra, collective flow, femtoscopy, light-nuclei production, net-proton fluctuations Anisotropic flow vn Flow correlations Balance functions Photons and dileptons Initial Fluctuation spectrum & baryon stoping Tµ⌫(⌧, r), Jµ(⌧, r) AAACGHicdVDJSgNBEO2JW4xb1KOXxiBECHEmippb0It4ipANMkno6fQkTXp6hl6EMOQzvPgrXjwo4jU3/8bOImjUBwWP96qoqudFjEpl2x9WYml5ZXUtuZ7a2Nza3knv7tVkqAUmVRyyUDQ8JAmjnFQVVYw0IkFQ4DFS9wbXE79+T4SkIa+oYURaAepx6lOMlJE66ZNKO3YD7XI9yroK6RyMXc+HYnScg7dt4yyonXTGzhdtp3juwN/EydtTZMAc5U567HZDrAPCFWZIyqZjR6oVI6EoZmSUcrUkEcID1CNNQzkKiGzF08dG8MgoXeiHwhRXcKp+n4hRIOUw8ExngFRfLnoT8S+vqZV/2Yopj7QiHM8W+ZpBFcJJSrBLBcGKDQ1BWFBzK8R9JBBWJsuUCeHrU/g/qRXyzmm+cHeWKV3N40iCA3AIssABF6AEbkAZVAEGD+AJvIBX69F6tt6s91lrwprP7IMfsMaf5XCfDg== Net particle distributions Critical point & 1st order PT Shear and bulk viscosities (η/s)(T, {μ q }), (ζ/s)(T, {μ q }) e(T, {μ q }), P(T, {μ q }), c2 s (T, {μ q }) 3

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 4 A long wavelength effective description of interacting systems Conservation laws + Equation of State Star formation Quark-Gluon Plasma Air dynamics of race car Studying collective phenomena in heavy-ion collisions has been leading the theory frontier of developing causal viscous relativistic hydrodynamics COLLECTIVITY & HYDRODYNAMICS

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 5 RUNNING THE GAMUT OF HIGH ENERGY NUCLEAR COLLISIONS B. Schenke, C. Shen and P. Tribedy, arXiv:2005.14682 [nucl-th] • One single set of model parameters for all types of collisions at the top RHIC and LHC energies LHC RHIC

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 6 QUANTITATIVE CHARACTERIZATION OF QGP 0.0 0.1 0.2 0.3 ¥/s LHC RHIC 2012 LHC RHIC 2015 2017-2018 latest lQCD EoS Duke-OSU (LHC) 2019 JETSCAPE (RHIC + LHC) 0.15 0.2 0.25 T (GeV) 0.0 0.1 0.2 0.3 ≥/s IPGlasma Trento Bayesian EKRT 0.15 0.2 0.25 T (GeV) 0.15 0.2 0.25 T (GeV) 0.15 0.2 0.25 T (GeV) Phys. Rev. Lett. 110, 012302 (2013) Phys. Rev. Lett. 115, 132301 (2015) Phys. Rev. C 93, 024907 (2016) C. Shen, arXiv:2001.11858 [nucl-th] Phenomenological constraints from top RHIC and LHC data

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 7 • Search for a critical point & 1st order phase transition • Access to new transport phenomena • How does the QGP transport property change with baryon doping? Charge diffusion , (η/s)(T, {μ q }) (ζ/s)(T, {μ q }) RHIC BES program QGP Hadron Gas LHC Neutron star merger FAIR/NICA HADES JPARC-HI PROBING THE NUCLEAR MATTER PHASE DIAGRAM

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 8 QCD EQUATION OF STATE AT FINITE DENSITIES A. Monnai, B. Schenke and C. Shen, Phys. Rev. C100, 024907 (2019) nS = 0 (null) (null) (null) (null) nQ = 0.4nB (null) (null) (null) (null) ns = 0 AAAB7nicbVDLSsNAFL2pr1pfUZduBovgqiRWfCyEohuXFewD2lAm00k7dDIJMxOhhH6EGxeKuPV73Pk3TtIgaj1w4XDOvdx7jx9zprTjfFqlpeWV1bXyemVjc2t7x97da6sokYS2SMQj2fWxopwJ2tJMc9qNJcWhz2nHn9xkfueBSsUica+nMfVCPBIsYARrI3XEQKEr5AzsqlNzcqBF4hakCgWaA/ujP4xIElKhCcdK9Vwn1l6KpWaE01mlnygaYzLBI9ozVOCQKi/Nz52hI6MMURBJU0KjXP05keJQqWnom84Q67H662Xif14v0cGFlzIRJ5oKMl8UJBzpCGW/oyGTlGg+NQQTycytiIyxxESbhCp5CJcZzr5fXiTtk5pbr9XvTquN6yKOMhzAIRyDC+fQgFtoQgsITOARnuHFiq0n69V6m7eWrGJmH37Bev8CGTyO5A== nQ = 0.4nB AAAB9HicbVBNS8NAEJ3Ur1q/qh69LBbBU0hs8eMglHrx2IK1hTaEzXbTLt1s4u6mUEp/hxcPinj1x3jz35ikQdT6YODx3gwz87yIM6Ut69MorKyurW8UN0tb2zu7e+X9g3sVxpLQNgl5KLseVpQzQduaaU67kaQ48DjteOOb1O9MqFQsFHd6GlEnwEPBfEawTiRHuC10jSyzhoTbcMsVy7QyoGVi56QCOZpu+aM/CEkcUKEJx0r1bCvSzgxLzQin81I/VjTCZIyHtJdQgQOqnFl29BydJMoA+aFMSmiUqT8nZjhQahp4SWeA9Uj99VLxP68Xa//SmTERxZoKsljkxxzpEKUJoAGTlGg+TQgmkiW3IjLCEhOd5FTKQrhKcf798jK5PzPtqllt1Sr1Rh5HEY7gGE7Bhguowy00oQ0EHuARnuHFmBhPxqvxtmgtGPnMIfyC8f4FMO6Qjw== Lattice QCD: Taylor expansion up to the 4th order Match to Hadron Resonance Gas model at low T P T4 = 1 2 [1 f(T, µJ )] Phad(T, µJ ) T4 + 1 2 [1 + f(T, µJ )] Plat(T, µJ ) T4 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 f(T, µB) = tanh[(T Tc(µB)/ Tc] AAACFXicdZDLSgMxFIYz9V5vVZdugkWoUOuMeF0IpbpwWaE36AxDJs3YYCYzJGeEUnwJN76KGxeKuBXc+TamF8HrD4Gf75zDyfmDRHANtv1uZSYmp6ZnZuey8wuLS8u5ldWGjlNFWZ3GIlatgGgmuGR14CBYK1GMRIFgzeDqdFBvXjOleSxr0EuYF5FLyUNOCRjk54phoVZ0o9SvbOET7AKR3Xahtl3zaWFEd9wzJoBgQzw/l7dLx7ZzfODg38Yp2UPl0VhVP/fmdmKaRkwCFUTrtmMn4PWJAk4Fu8m6qWYJoVfkkrWNlSRi2usPr7rBm4Z0cBgr8yTgIf060SeR1r0oMJ0Rga7+WRvAv2rtFMIjr89lkgKTdLQoTAWGGA8iwh2uGAXRM4ZQxc1fMe0SRSiYILMmhM9L8f+msVty9kr7F3v5cmUcxyxaRxuogBx0iMroHFVRHVF0i+7RI3qy7qwH69l6GbVmrPHMGvom6/UDl0GcpQ== Tc(µB) = 0.16 GeV 0.4(0.139 GeV 1µ2 B + 0.053 GeV 3µ4 B ) 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 Tc = 0.1Tc(µB = 0) AAACCHicdVDLSsNAFJ34rPUVdenCwSLUTUikProQSnXhskJf0IQwmU7boTNJmJkIJXTpxl9x40IRt36CO//GSVvB54ELZ865l7n3BDGjUtn2uzE3v7C4tJxbya+urW9smlvbTRklApMGjlgk2gGShNGQNBRVjLRjQRAPGGkFw4vMb90QIWkU1tUoJh5H/ZD2KEZKS765514SphCs+xieQ9tyMlZ0eeJXs/ehbxZsq2w75RMH/iaOZU9QADPUfPPN7UY44SRUmCEpO44dKy9FQlHMyDjvJpLECA9Rn3Q0DREn0ksnh4zhgVa6sBcJXaGCE/XrRIq4lCMe6E6O1ED+9DLxL6+TqN6Zl9IwThQJ8fSjXsKgimCWCuxSQbBiI00QFlTvCvEACYSVzi6vQ/i8FP5PmkeWU7KOr0uFSnUWRw7sgn1QBA44BRVwBWqgATC4BffgETwZd8aD8Wy8TFvnjNnMDvgG4/UDCjiW0g== M. Albright, J. Kapusta and C. Young, Phys. Rev. C90, 024915 (2014) J. Noronha-Hostler, P. Parotto, C. Ratti and J. M. Stafford, Phys. Rev. C100, 064910 (2019)

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 9 QCD EQUATION OF STATE AT FINITE DENSITIES • Strangeness neutrality improves the hadronic chemistry in the hybrid dynamic framework nS = 0 (null) (null) (null) (null) nQ = 0.4nB (null) (null) (null) (null) 0.1 0.2 0.3 T (GeV) 0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35 c2 s p sNN = 200 GeV p sNN = 62.4 GeV p sNN = 19.6 GeV p sNN = 14.5 GeV c2 s AAAB7HicbVBNS8NAEJ34WetX1aOXxSJ4KkkrftyKXjxWMG2hjWWz3bRLN5uwuxFK6G/w4kERr/4gb/4bN2kQtT4YeLw3w8w8P+ZMadv+tJaWV1bX1ksb5c2t7Z3dyt5+W0WJJNQlEY9k18eKciaoq5nmtBtLikOf044/uc78zgOVikXiTk9j6oV4JFjACNZGcslA3dcHlapds3OgReIUpAoFWoPKR38YkSSkQhOOleo5dqy9FEvNCKezcj9RNMZkgke0Z6jAIVVemh87Q8dGGaIgkqaERrn6cyLFoVLT0DedIdZj9dfLxP+8XqKDCy9lIk40FWS+KEg40hHKPkdDJinRfGoIJpKZWxEZY4mJNvmU8xAuM5x9v7xI2vWa06g1bk+rzasijhIcwhGcgAPn0IQbaIELBBg8wjO8WMJ6sl6tt3nrklXMHMAvWO9fj2uOqA== ns = 0 AAAB7nicbVDLSsNAFL2pr1pfUZduBovgqiRWfCyEohuXFewD2lAm00k7dDIJMxOhhH6EGxeKuPV73Pk3TtIgaj1w4XDOvdx7jx9zprTjfFqlpeWV1bXyemVjc2t7x97da6sokYS2SMQj2fWxopwJ2tJMc9qNJcWhz2nHn9xkfueBSsUica+nMfVCPBIsYARrI3XEQKEr5AzsqlNzcqBF4hakCgWaA/ujP4xIElKhCcdK9Vwn1l6KpWaE01mlnygaYzLBI9ozVOCQKi/Nz52hI6MMURBJU0KjXP05keJQqWnom84Q67H662Xif14v0cGFlzIRJ5oKMl8UJBzpCGW/oyGTlGg+NQQTycytiIyxxESbhCp5CJcZzr5fXiTtk5pbr9XvTquN6yKOMhzAIRyDC+fQgFtoQgsITOARnuHFiq0n69V6m7eWrGJmH37Bev8CGTyO5A== nQ = 0.4nB AAAB9HicbVBNS8NAEJ3Ur1q/qh69LBbBU0hs8eMglHrx2IK1hTaEzXbTLt1s4u6mUEp/hxcPinj1x3jz35ikQdT6YODx3gwz87yIM6Ut69MorKyurW8UN0tb2zu7e+X9g3sVxpLQNgl5KLseVpQzQduaaU67kaQ48DjteOOb1O9MqFQsFHd6GlEnwEPBfEawTiRHuC10jSyzhoTbcMsVy7QyoGVi56QCOZpu+aM/CEkcUKEJx0r1bCvSzgxLzQin81I/VjTCZIyHtJdQgQOqnFl29BydJMoA+aFMSmiUqT8nZjhQahp4SWeA9Uj99VLxP68Xa//SmTERxZoKsljkxxzpEKUJoAGTlGg+TQgmkiW3IjLCEhOd5FTKQrhKcf798jK5PzPtqllt1Sr1Rh5HEY7gGE7Bhguowy00oQ0EHuARnuHFmBhPxqvxtmgtGPnMIfyC8f4FMO6Qjw== A. Monnai, B. Schenke and C. Shen, Phys. Rev. C100, 024907 (2019) https://sites.google.com/view/qcdneos/ Enabled hydrodynamic simulations at finite μ

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 10 QCD EQUATION OF STATE AT FINITE DENSITIES • Strangeness neutrality improves the hadronic chemistry in the hybrid dynamic framework nS = 0 (null) (null) (null) (null) nQ = 0.4nB (null) (null) (null) (null) 0.1 0.2 0.3 T (GeV) 0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35 c2 s p sNN = 200 GeV p sNN = 62.4 GeV p sNN = 19.6 GeV p sNN = 14.5 GeV c2 s AAAB7HicbVBNS8NAEJ34WetX1aOXxSJ4KkkrftyKXjxWMG2hjWWz3bRLN5uwuxFK6G/w4kERr/4gb/4bN2kQtT4YeLw3w8w8P+ZMadv+tJaWV1bX1ksb5c2t7Z3dyt5+W0WJJNQlEY9k18eKciaoq5nmtBtLikOf044/uc78zgOVikXiTk9j6oV4JFjACNZGcslA3dcHlapds3OgReIUpAoFWoPKR38YkSSkQhOOleo5dqy9FEvNCKezcj9RNMZkgke0Z6jAIVVemh87Q8dGGaIgkqaERrn6cyLFoVLT0DedIdZj9dfLxP+8XqKDCy9lIk40FWS+KEg40hHKPkdDJinRfGoIJpKZWxEZY4mJNvmU8xAuM5x9v7xI2vWa06g1bk+rzasijhIcwhGcgAPn0IQbaIELBBg8wjO8WMJ6sl6tt3nrklXMHMAvWO9fj2uOqA== ns = 0 AAAB7nicbVDLSsNAFL2pr1pfUZduBovgqiRWfCyEohuXFewD2lAm00k7dDIJMxOhhH6EGxeKuPV73Pk3TtIgaj1w4XDOvdx7jx9zprTjfFqlpeWV1bXyemVjc2t7x97da6sokYS2SMQj2fWxopwJ2tJMc9qNJcWhz2nHn9xkfueBSsUica+nMfVCPBIsYARrI3XEQKEr5AzsqlNzcqBF4hakCgWaA/ujP4xIElKhCcdK9Vwn1l6KpWaE01mlnygaYzLBI9ozVOCQKi/Nz52hI6MMURBJU0KjXP05keJQqWnom84Q67H662Xif14v0cGFlzIRJ5oKMl8UJBzpCGW/oyGTlGg+NQQTycytiIyxxESbhCp5CJcZzr5fXiTtk5pbr9XvTquN6yKOMhzAIRyDC+fQgFtoQgsITOARnuHFiq0n69V6m7eWrGJmH37Bev8CGTyO5A== nQ = 0.4nB AAAB9HicbVBNS8NAEJ3Ur1q/qh69LBbBU0hs8eMglHrx2IK1hTaEzXbTLt1s4u6mUEp/hxcPinj1x3jz35ikQdT6YODx3gwz87yIM6Ut69MorKyurW8UN0tb2zu7e+X9g3sVxpLQNgl5KLseVpQzQduaaU67kaQ48DjteOOb1O9MqFQsFHd6GlEnwEPBfEawTiRHuC10jSyzhoTbcMsVy7QyoGVi56QCOZpu+aM/CEkcUKEJx0r1bCvSzgxLzQin81I/VjTCZIyHtJdQgQOqnFl29BydJMoA+aFMSmiUqT8nZjhQahp4SWeA9Uj99VLxP68Xa//SmTERxZoKsljkxxzpEKUJoAGTlGg+TQgmkiW3IjLCEhOd5FTKQrhKcf798jK5PzPtqllt1Sr1Rh5HEY7gGE7Bhguowy00oQ0EHuARnuHFmBhPxqvxtmgtGPnMIfyC8f4FMO6Qjw== A. Monnai, B. Schenke and C. Shen, Phys. Rev. C100, 024907 (2019) https://sites.google.com/view/qcdneos/ Enabled hydrodynamic simulations at finite μ

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 11 • Classical string-based initial conditions • Transport model based initial conditions A. Bialas, A. Bzdak and V. Koch, Acta Phys. Polon. B49 (2018) C. Shen and B. Schenke, Phys.Rev. C97 (2018) 024907 time L. Du, U. Heinz and G. Vujanovic, Nucl. Phys. A982 (2019) 407-410 I. A. Karpenko, P. Huovinen, H. Petersen and M. Bleicher, Phys. Rev. C91 (2015) 064901 3D DYNAMICS BEYOND THE BJORKEN PARADIGM • Color Glass Condensate based models L. D. McLerran, S. Schlichting and S. Sen, Phys. Rev. D 99, 074009 (2019) M. Li and J. Kapusta, Phys. Rev. C 99, 014906 (2019) • Holographic approach at intermediate coupling M. Attems, et al., Phys.Rev.Lett. 121 (2018), 261601 • Geometry-Based initial conditions C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020) M. Martinez, M. D. Sievert, D. E. Wertepny and J. Noronha-Hostler, arXiv:1911.10272 + arXiv:1911.12454 [nucl-th]

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 12 A MINIMUM EXTENSION TO 3D INITIAL CONDITIONS • Impose energy and momentum conservation on the Glauber geometry Assumption: All of the energy and momentum is deposited into the medium C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020) • Assume Bjorken flow for the velocity profile uμ init = (cosh(η s ),0,0, sinh(η s )) • Energy density given by a longitudinal flux-tube profile where e (x, y) ∝ M(x, y) • For the local energy density s ≥ 5 GeV, e(x, y) ∝ T A T B

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 13 C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020) A MINIMUM EXTENSION TO 3D INITIAL CONDITIONS

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 14 ⌧ ⌘ t z p sNN = 200 GeV Calibration Model extrapolation 0 50 100 150 200 dNº° /dy 0-5% (a) 5-12.5% (b) 12.5-23.5% (c) °6 °3 0 3 6 y 0 25 50 75 dNº° /dy 23.5-33.5% (d) °6 °3 0 3 6 y 33.5-43.5% (e) °6 °3 0 3 6 y Pb+Pb @ SPS 17.3 GeV 8.77 GeV Calibration Model extrapolation PARTICLE PRODUCTIONS AT RHIC BES AND SPS C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020) • Centrality dependence of particle production can be well reproduced

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 15 PARTICLE RAPIDITY DISTRIBUTION AT RHIC BES • With limited data from RHIC BES I, we make predictions for the rapidity dependence of particle productions C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020)

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 16 PARTICLE PRODUCTIONS AT RHIC BES AND SPS C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020) • Imposing energy-momentum conservation is extremely important for making predictions for asymmetric d+Au collisions °6 °4 °2 0 2 4 6 ¥ 0 5 10 15 20 25 30 35 dNch/d¥ 0-5% dAu@ 200 GeV 0-5% dAu@ 62.4 GeV 0-10% dAu@ 39 GeV 0-20% dAu@ 19.6 GeV °6 °4 °2 0 2 4 6 ¥ 0 20 40 60 80 dNch/d¥ no momentum conservation with momentum conservation PHENIX 0-5% dAu @ 200 GeV

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 17 COLLISION ENERGY DEPENDENT RADIAL FLOW • Identified particles mean are reproduced as a function of p T s • The absent of pre-equilibrium dynamics suggests non-zero bulk viscosity ζ/s(T, μ B ) C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020)

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 18 COLLISION ENERGY DEPENDENT RADIAL FLOW • Identified particles mean are reproduced as a function of p T s • The absent of pre-equilibrium dynamics suggests non-zero bulk viscosity ζ/s(T, μ B ) C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020)

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 19 RAPIDITY DEPENDENT DIRECT FLOW C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020) • The direct flow of agree reasonably with the measurements π ∝ ε 1 (e) • The direct flow of are over predicted p ∝ ε 1 (n B )

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 20 ELLIPTIC FLOW AT RHIC BES AND SHEAR VISCOSITY C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020) • The rapidity and centrality dependence of v2 can set strong constraints on the (η/s)(T, μ B ) I. A. Karpenko, P. Huovinen, H. Petersen and M. Bleicher, Phys. Rev. C91 (2015) 064901

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 21 HBT RADII AT THE RHIC BES Based on C. Shen and S. Alzhrani, Phys. Rev. C 102, 014909 (2020) 101 102 p s (GeV) 0 1 2 3 4 5 6 7 R (fm) Rout Rside p R2 out ° R2 side STAR Rout STAR Rside STAR p R2 out ° R2 side 101 102 p s (GeV) 0 1 2 3 4 5 6 7 8 R (fm) Rlong STAR Rlong • The model reasonably describe the collision energy dependence of Rout and Rside; Rlong is overestimated and need further investigation • is flat vs. ; no non-monotonic behavior in the model R2 out − R2 side s Preliminary Preliminary

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 22 THE 3D MC-GLAUBER + STRING MODEL C. Shen and B. Schenke, Phys.Rev. C97 (2018) 024907 t Pair rest frame yi yi yf yf

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 23 C. Shen and B. Schenke, Phys.Rev. C97 (2018) 024907 t Pair rest frame yi yi yf yf ηs energy density inside the string yCM THE 3D MC-GLAUBER + STRING MODEL

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 24 C. Shen and B. Schenke, Phys.Rev. C97 (2018) 024907 t Pair rest frame yi yi yf yf ηs energy density inside the string yCM ηs yCM net baryon density and energy density at the string ends THE 3D MC-GLAUBER + STRING MODEL

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 25 C. Shen and B. Schenke, Phys.Rev. C97 (2018) 024907 t Pair rest frame yi yi yf yf ηs energy density inside the string yCM ηs yCM Baryon density are deposited at the string ends or string junctions D. Kharzeev, Phys. Lett. B 378, 238 (1996) THE 3D MC-GLAUBER + STRING MODEL

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 26 C. Shen and B. Schenke, Phys.Rev. C97 (2018) 024907 t Pair rest frame yi yi yf yf ηs energy density inside the string yCM ηs yCM Baryon density are deposited at the string ends or string junctions D. Kharzeev, Phys. Lett. B 378, 238 (1996) Imposed conservation for energy, momentum, and net baryon density THE 3D MC-GLAUBER + STRING MODEL

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 27 °5.0 °2.5 0.0 2.5 5.0 ¥s 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 ø (fm) 0-5% Au+Au @ 200 GeV °5.0 °2.5 0.0 2.5 5.0 z (fm) 0 1 2 3 4 5 t (fm) 0-5% Au+Au @ 200 GeV t z STRINGS’ SPACE-TIME DISTRIBUTION ⌘s = 0 AAAB8HicbVBNS8NAEN3Ur1q/qh69LBbBU0lEUA9C0YvHCsYW21A220m7dLMJuxOhhP4LLx5UvPpzvPlv3LY5aPXBwOO9GWbmhakUBl33yyktLa+srpXXKxubW9s71d29e5NkmoPPE5nodsgMSKHAR4ES2qkGFocSWuHoeuq3HkEbkag7HKcQxGygRCQ4Qys9dAFZz9BL6vaqNbfuzkD/Eq8gNVKg2at+dvsJz2JQyCUzpuO5KQY50yi4hEmlmxlIGR+xAXQsVSwGE+Sziyf0yCp9GiXalkI6U39O5Cw2ZhyHtjNmODSL3lT8z+tkGJ0HuVBphqD4fFGUSYoJnb5P+0IDRzm2hHEt7K2UD5lmHG1IFRuCt/jyX+Kf1C/q3u1prXFVpFEmB+SQHBOPnJEGuSFN4hNOFHkiL+TVMc6z8+a8z1tLTjGzT37B+fgGpPuPxw== AAAB8HicbVBNS8NAEN3Ur1q/qh69LBbBU0lEUA9C0YvHCsYW21A220m7dLMJuxOhhP4LLx5UvPpzvPlv3LY5aPXBwOO9GWbmhakUBl33yyktLa+srpXXKxubW9s71d29e5NkmoPPE5nodsgMSKHAR4ES2qkGFocSWuHoeuq3HkEbkag7HKcQxGygRCQ4Qys9dAFZz9BL6vaqNbfuzkD/Eq8gNVKg2at+dvsJz2JQyCUzpuO5KQY50yi4hEmlmxlIGR+xAXQsVSwGE+Sziyf0yCp9GiXalkI6U39O5Cw2ZhyHtjNmODSL3lT8z+tkGJ0HuVBphqD4fFGUSYoJnb5P+0IDRzm2hHEt7K2UD5lmHG1IFRuCt/jyX+Kf1C/q3u1prXFVpFEmB+SQHBOPnJEGuSFN4hNOFHkiL+TVMc6z8+a8z1tLTjGzT37B+fgGpPuPxw== AAAB8HicbVBNS8NAEN3Ur1q/qh69LBbBU0lEUA9C0YvHCsYW21A220m7dLMJuxOhhP4LLx5UvPpzvPlv3LY5aPXBwOO9GWbmhakUBl33yyktLa+srpXXKxubW9s71d29e5NkmoPPE5nodsgMSKHAR4ES2qkGFocSWuHoeuq3HkEbkag7HKcQxGygRCQ4Qys9dAFZz9BL6vaqNbfuzkD/Eq8gNVKg2at+dvsJz2JQyCUzpuO5KQY50yi4hEmlmxlIGR+xAXQsVSwGE+Sziyf0yCp9GiXalkI6U39O5Cw2ZhyHtjNmODSL3lT8z+tkGJ0HuVBphqD4fFGUSYoJnb5P+0IDRzm2hHEt7K2UD5lmHG1IFRuCt/jyX+Kf1C/q3u1prXFVpFEmB+SQHBOPnJEGuSFN4hNOFHkiL+TVMc6z8+a8z1tLTjGzT37B+fgGpPuPxw== AAAB8HicbVBNS8NAEN3Ur1q/qh69LBbBU0lEUA9C0YvHCsYW21A220m7dLMJuxOhhP4LLx5UvPpzvPlv3LY5aPXBwOO9GWbmhakUBl33yyktLa+srpXXKxubW9s71d29e5NkmoPPE5nodsgMSKHAR4ES2qkGFocSWuHoeuq3HkEbkag7HKcQxGygRCQ4Qys9dAFZz9BL6vaqNbfuzkD/Eq8gNVKg2at+dvsJz2JQyCUzpuO5KQY50yi4hEmlmxlIGR+xAXQsVSwGE+Sziyf0yCp9GiXalkI6U39O5Cw2ZhyHtjNmODSL3lT8z+tkGJ0HuVBphqD4fFGUSYoJnb5P+0IDRzm2hHEt7K2UD5lmHG1IFRuCt/jyX+Kf1C/q3u1prXFVpFEmB+SQHBOPnJEGuSFN4hNOFHkiL+TVMc6z8+a8z1tLTjGzT37B+fgGpPuPxw== ⌘s = 3 AAAB8HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lUUA9C0YvHCsYW21A222m7dLMJuxuhhP4LLx5UvPpzvPlv3LY5aOuDgcd7M8zMCxPBtXHdb6ewtLyyulZcL21sbm3vlHf3HnScKoY+i0WsmiHVKLhE33AjsJkopFEosBEObyZ+4wmV5rG8N6MEg4j2Je9xRo2VHttoaEeTK3LaKVfcqjsFWSReTiqQo94pf7W7MUsjlIYJqnXLcxMTZFQZzgSOS+1UY0LZkPaxZamkEeogm148JkdW6ZJerGxJQ6bq74mMRlqPotB2RtQM9Lw3Ef/zWqnpXQQZl0lqULLZol4qiInJ5H3S5QqZESNLKFPc3krYgCrKjA2pZEPw5l9eJP5J9bLq3Z1Vatd5GkU4gEM4Bg/OoQa3UAcfGEh4hld4c7Tz4rw7H7PWgpPP7MMfOJ8/qYSPyg== AAAB8HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lUUA9C0YvHCsYW21A222m7dLMJuxuhhP4LLx5UvPpzvPlv3LY5aOuDgcd7M8zMCxPBtXHdb6ewtLyyulZcL21sbm3vlHf3HnScKoY+i0WsmiHVKLhE33AjsJkopFEosBEObyZ+4wmV5rG8N6MEg4j2Je9xRo2VHttoaEeTK3LaKVfcqjsFWSReTiqQo94pf7W7MUsjlIYJqnXLcxMTZFQZzgSOS+1UY0LZkPaxZamkEeogm148JkdW6ZJerGxJQ6bq74mMRlqPotB2RtQM9Lw3Ef/zWqnpXQQZl0lqULLZol4qiInJ5H3S5QqZESNLKFPc3krYgCrKjA2pZEPw5l9eJP5J9bLq3Z1Vatd5GkU4gEM4Bg/OoQa3UAcfGEh4hld4c7Tz4rw7H7PWgpPP7MMfOJ8/qYSPyg== AAAB8HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lUUA9C0YvHCsYW21A222m7dLMJuxuhhP4LLx5UvPpzvPlv3LY5aOuDgcd7M8zMCxPBtXHdb6ewtLyyulZcL21sbm3vlHf3HnScKoY+i0WsmiHVKLhE33AjsJkopFEosBEObyZ+4wmV5rG8N6MEg4j2Je9xRo2VHttoaEeTK3LaKVfcqjsFWSReTiqQo94pf7W7MUsjlIYJqnXLcxMTZFQZzgSOS+1UY0LZkPaxZamkEeogm148JkdW6ZJerGxJQ6bq74mMRlqPotB2RtQM9Lw3Ef/zWqnpXQQZl0lqULLZol4qiInJ5H3S5QqZESNLKFPc3krYgCrKjA2pZEPw5l9eJP5J9bLq3Z1Vatd5GkU4gEM4Bg/OoQa3UAcfGEh4hld4c7Tz4rw7H7PWgpPP7MMfOJ8/qYSPyg== AAAB8HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lUUA9C0YvHCsYW21A222m7dLMJuxuhhP4LLx5UvPpzvPlv3LY5aOuDgcd7M8zMCxPBtXHdb6ewtLyyulZcL21sbm3vlHf3HnScKoY+i0WsmiHVKLhE33AjsJkopFEosBEObyZ+4wmV5rG8N6MEg4j2Je9xRo2VHttoaEeTK3LaKVfcqjsFWSReTiqQo94pf7W7MUsjlIYJqnXLcxMTZFQZzgSOS+1UY0LZkPaxZamkEeogm148JkdW6ZJerGxJQ6bq74mMRlqPotB2RtQM9Lw3Ef/zWqnpXQQZl0lqULLZol4qiInJ5H3S5QqZESNLKFPc3krYgCrKjA2pZEPw5l9eJP5J9bLq3Z1Vatd5GkU4gEM4Bg/OoQa3UAcfGEh4hld4c7Tz4rw7H7PWgpPP7MMfOJ8/qYSPyg== °5.0 °2.5 0.0 2.5 5.0 z (fm) 0 1 2 3 4 5 t (fm) 0-5% Au+Au @ 19.6 GeV °5.0 °2.5 0.0 2.5 5.0 ¥s 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 ø (fm) 0-5% Au+Au @ 19.6 GeV ⌘s = 0 AAAB8HicbVBNS8NAEN3Ur1q/qh69LBbBU0lEUA9C0YvHCsYW21A220m7dLMJuxOhhP4LLx5UvPpzvPlv3LY5aPXBwOO9GWbmhakUBl33yyktLa+srpXXKxubW9s71d29e5NkmoPPE5nodsgMSKHAR4ES2qkGFocSWuHoeuq3HkEbkag7HKcQxGygRCQ4Qys9dAFZz9BL6vaqNbfuzkD/Eq8gNVKg2at+dvsJz2JQyCUzpuO5KQY50yi4hEmlmxlIGR+xAXQsVSwGE+Sziyf0yCp9GiXalkI6U39O5Cw2ZhyHtjNmODSL3lT8z+tkGJ0HuVBphqD4fFGUSYoJnb5P+0IDRzm2hHEt7K2UD5lmHG1IFRuCt/jyX+Kf1C/q3u1prXFVpFEmB+SQHBOPnJEGuSFN4hNOFHkiL+TVMc6z8+a8z1tLTjGzT37B+fgGpPuPxw== AAAB8HicbVBNS8NAEN3Ur1q/qh69LBbBU0lEUA9C0YvHCsYW21A220m7dLMJuxOhhP4LLx5UvPpzvPlv3LY5aPXBwOO9GWbmhakUBl33yyktLa+srpXXKxubW9s71d29e5NkmoPPE5nodsgMSKHAR4ES2qkGFocSWuHoeuq3HkEbkag7HKcQxGygRCQ4Qys9dAFZz9BL6vaqNbfuzkD/Eq8gNVKg2at+dvsJz2JQyCUzpuO5KQY50yi4hEmlmxlIGR+xAXQsVSwGE+Sziyf0yCp9GiXalkI6U39O5Cw2ZhyHtjNmODSL3lT8z+tkGJ0HuVBphqD4fFGUSYoJnb5P+0IDRzm2hHEt7K2UD5lmHG1IFRuCt/jyX+Kf1C/q3u1prXFVpFEmB+SQHBOPnJEGuSFN4hNOFHkiL+TVMc6z8+a8z1tLTjGzT37B+fgGpPuPxw== AAAB8HicbVBNS8NAEN3Ur1q/qh69LBbBU0lEUA9C0YvHCsYW21A220m7dLMJuxOhhP4LLx5UvPpzvPlv3LY5aPXBwOO9GWbmhakUBl33yyktLa+srpXXKxubW9s71d29e5NkmoPPE5nodsgMSKHAR4ES2qkGFocSWuHoeuq3HkEbkag7HKcQxGygRCQ4Qys9dAFZz9BL6vaqNbfuzkD/Eq8gNVKg2at+dvsJz2JQyCUzpuO5KQY50yi4hEmlmxlIGR+xAXQsVSwGE+Sziyf0yCp9GiXalkI6U39O5Cw2ZhyHtjNmODSL3lT8z+tkGJ0HuVBphqD4fFGUSYoJnb5P+0IDRzm2hHEt7K2UD5lmHG1IFRuCt/jyX+Kf1C/q3u1prXFVpFEmB+SQHBOPnJEGuSFN4hNOFHkiL+TVMc6z8+a8z1tLTjGzT37B+fgGpPuPxw== AAAB8HicbVBNS8NAEN3Ur1q/qh69LBbBU0lEUA9C0YvHCsYW21A220m7dLMJuxOhhP4LLx5UvPpzvPlv3LY5aPXBwOO9GWbmhakUBl33yyktLa+srpXXKxubW9s71d29e5NkmoPPE5nodsgMSKHAR4ES2qkGFocSWuHoeuq3HkEbkag7HKcQxGygRCQ4Qys9dAFZz9BL6vaqNbfuzkD/Eq8gNVKg2at+dvsJz2JQyCUzpuO5KQY50yi4hEmlmxlIGR+xAXQsVSwGE+Sziyf0yCp9GiXalkI6U39O5Cw2ZhyHtjNmODSL3lT8z+tkGJ0HuVBphqD4fFGUSYoJnb5P+0IDRzm2hHEt7K2UD5lmHG1IFRuCt/jyX+Kf1C/q3u1prXFVpFEmB+SQHBOPnJEGuSFN4hNOFHkiL+TVMc6z8+a8z1tLTjGzT37B+fgGpPuPxw== ⌘s = 3 AAAB8HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lUUA9C0YvHCsYW21A222m7dLMJuxuhhP4LLx5UvPpzvPlv3LY5aOuDgcd7M8zMCxPBtXHdb6ewtLyyulZcL21sbm3vlHf3HnScKoY+i0WsmiHVKLhE33AjsJkopFEosBEObyZ+4wmV5rG8N6MEg4j2Je9xRo2VHttoaEeTK3LaKVfcqjsFWSReTiqQo94pf7W7MUsjlIYJqnXLcxMTZFQZzgSOS+1UY0LZkPaxZamkEeogm148JkdW6ZJerGxJQ6bq74mMRlqPotB2RtQM9Lw3Ef/zWqnpXQQZl0lqULLZol4qiInJ5H3S5QqZESNLKFPc3krYgCrKjA2pZEPw5l9eJP5J9bLq3Z1Vatd5GkU4gEM4Bg/OoQa3UAcfGEh4hld4c7Tz4rw7H7PWgpPP7MMfOJ8/qYSPyg== AAAB8HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lUUA9C0YvHCsYW21A222m7dLMJuxuhhP4LLx5UvPpzvPlv3LY5aOuDgcd7M8zMCxPBtXHdb6ewtLyyulZcL21sbm3vlHf3HnScKoY+i0WsmiHVKLhE33AjsJkopFEosBEObyZ+4wmV5rG8N6MEg4j2Je9xRo2VHttoaEeTK3LaKVfcqjsFWSReTiqQo94pf7W7MUsjlIYJqnXLcxMTZFQZzgSOS+1UY0LZkPaxZamkEeogm148JkdW6ZJerGxJQ6bq74mMRlqPotB2RtQM9Lw3Ef/zWqnpXQQZl0lqULLZol4qiInJ5H3S5QqZESNLKFPc3krYgCrKjA2pZEPw5l9eJP5J9bLq3Z1Vatd5GkU4gEM4Bg/OoQa3UAcfGEh4hld4c7Tz4rw7H7PWgpPP7MMfOJ8/qYSPyg== AAAB8HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lUUA9C0YvHCsYW21A222m7dLMJuxuhhP4LLx5UvPpzvPlv3LY5aOuDgcd7M8zMCxPBtXHdb6ewtLyyulZcL21sbm3vlHf3HnScKoY+i0WsmiHVKLhE33AjsJkopFEosBEObyZ+4wmV5rG8N6MEg4j2Je9xRo2VHttoaEeTK3LaKVfcqjsFWSReTiqQo94pf7W7MUsjlIYJqnXLcxMTZFQZzgSOS+1UY0LZkPaxZamkEeogm148JkdW6ZJerGxJQ6bq74mMRlqPotB2RtQM9Lw3Ef/zWqnpXQQZl0lqULLZol4qiInJ5H3S5QqZESNLKFPc3krYgCrKjA2pZEPw5l9eJP5J9bLq3Z1Vatd5GkU4gEM4Bg/OoQa3UAcfGEh4hld4c7Tz4rw7H7PWgpPP7MMfOJ8/qYSPyg== AAAB8HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lUUA9C0YvHCsYW21A222m7dLMJuxuhhP4LLx5UvPpzvPlv3LY5aOuDgcd7M8zMCxPBtXHdb6ewtLyyulZcL21sbm3vlHf3HnScKoY+i0WsmiHVKLhE33AjsJkopFEosBEObyZ+4wmV5rG8N6MEg4j2Je9xRo2VHttoaEeTK3LaKVfcqjsFWSReTiqQo94pf7W7MUsjlIYJqnXLcxMTZFQZzgSOS+1UY0LZkPaxZamkEeogm148JkdW6ZJerGxJQ6bq74mMRlqPotB2RtQM9Lw3Ef/zWqnpXQQZl0lqULLZol4qiInJ5H3S5QqZESNLKFPc3krYgCrKjA2pZEPw5l9eJP5J9bLq3Z1Vatd5GkU4gEM4Bg/OoQa3UAcfGEh4hld4c7Tz4rw7H7PWgpPP7MMfOJ8/qYSPyg== ⌧ ⌘s AAAB9HicbVDLSgNBEJyNrxhfUY9eBoPgxbArET0GvXiMYB6QXULvZDYZMvtwpjcQlnyHFw+KePVjvPk3TpI9aGJBQ1HVTXeXn0ih0ba/rcLa+sbmVnG7tLO7t39QPjxq6ThVjDdZLGPV8UFzKSLeRIGSdxLFIfQlb/uju5nfHnOlRRw94iThXgiDSASCARrJcxFSekFdjtDTvXLFrtpz0FXi5KRCcjR65S+3H7M05BEyCVp3HTtBLwOFgkk+Lbmp5gmwEQx419AIQq69bH70lJ4ZpU+DWJmKkM7V3xMZhFpPQt90hoBDvezNxP+8borBjZeJKEmRR2yxKEglxZjOEqB9oThDOTEEmBLmVsqGoIChyalkQnCWX14lrcuqU6tePdQq9ds8jiI5IafknDjkmtTJPWmQJmHkiTyTV/Jmja0X6936WLQWrHzmmPyB9fkD0xSRfw== τ = t2 − z2 η s = 1 2 ln t + z t − z

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 28 HYDRODYNAMICS WITH SOURCES Energy-momentum current and net baryon density are fed into hydrodynamic simulation as source terms @µTµ⌫ = J⌫ source 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 @µJµ = ⇢source 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 AAACPXicdVDLSgMxFM34rPVVdekmWAQXMmTUUWchFN2IqwqtCjNjyaRpG5p5kGSEMsyPufEf3Llz40IRt27NtBV8Xgg5nHvuzckJEs6kQujBmJicmp6ZLc2V5xcWl5YrK6sXMk4FoU0S81hcBVhSziLaVExxepUIisOA08ugf1L0L2+okCyOGmqQUD/E3Yh1GMFKU61Kw0uwUAzzlhem8Ow601cOj2DmDXe7ohv4GTKR7dgW2kamjSxntwCOc7hn27knerEexaonwmzkKs9blaoWaOW+BX8Dy0TDqoJx1VuVe68dkzSkkSIcS+laKFF+VjgjnOZlL5U0waSPu9TVMMIhlX42dJjDTc20YScW+kQKDtmvExkOpRyEgVYWPuXPXkH+1XNT1Tn0MxYlqaIRGT3USTlUMSyihG0mKFF8oAEmgmmvkPSwwETpwMs6hM+fwv/BxY5pIdM636vWjsdxlMA62ABbwAIHoAZOQR00AQG34BE8gxfjzngyXo23kXTCGM+sgW9lvH8AtlKskg== 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 AAACPXicdVDLSgMxFM34rPVVdekmWAQXMmTUUWchFN2IqwqtCjNjyaRpG5p5kGSEMsyPufEf3Llz40IRt27NtBV8Xgg5nHvuzckJEs6kQujBmJicmp6ZLc2V5xcWl5YrK6sXMk4FoU0S81hcBVhSziLaVExxepUIisOA08ugf1L0L2+okCyOGmqQUD/E3Yh1GMFKU61Kw0uwUAzzlhem8Ow601cOj2DmDXe7ohv4GTKR7dgW2kamjSxntwCOc7hn27knerEexaonwmzkKs9blaoWaOW+BX8Dy0TDqoJx1VuVe68dkzSkkSIcS+laKFF+VjgjnOZlL5U0waSPu9TVMMIhlX42dJjDTc20YScW+kQKDtmvExkOpRyEgVYWPuXPXkH+1XNT1Tn0MxYlqaIRGT3USTlUMSyihG0mKFF8oAEmgmmvkPSwwETpwMs6hM+fwv/BxY5pIdM636vWjsdxlMA62ABbwAIHoAZOQR00AQG34BE8gxfjzngyXo23kXTCGM+sgW9lvH8AtlKskg== C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 L. Du, U. Heinz and G. Vujanovic, Nucl. Phys. A982 (2019) 407-410 M. Okai, K. Kawaguchi, Y. Tachibana, and T. Hirano, Phys. Rev. C95, 054914 (2017) z t Hydrodynamics Dynamical Initialization Hadron Transport

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 29 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 30 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 31 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=0.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 32 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=0.8 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 33 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=0.9 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 34 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=1.0 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 35 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=1.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 36 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=2.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 37 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=3.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 38 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=5.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 39 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=6.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 40 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=7.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 41 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=9.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 42 HYDRODYNAMICAL EVOLUTION WITH SOURCES C. Shen and B. Schenke, Phys. Rev. C97 (2018) 024907 p sNN = 19.6 GeV AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u AAACEnicdVDLSsNAFJ34rPUVdelmsAgKEhKRahdC0YWuSgX7gCaEyXTSDp08nJkIJeQb3Pgrblwo4taVO//GSR/g88CFwzn3cu89XsyokKb5oc3Mzs0vLBaWissrq2vr+sZmU0QJx6SBIxbxtocEYTQkDUklI+2YExR4jLS8wXnut24JFzQKr+UwJk6AeiH1KUZSSa6+b4sbLlPh2gGSfR6ktVqWwVNoVYyyfTAVL0gzc/WSaVRMq1K24G9iGeYIJTBB3dXf7W6Ek4CEEjMkRMcyY+mkiEuKGcmKdiJIjPAA9UhH0RAFRDjp6KUM7iqlC/2IqwolHKlfJ1IUCDEMPNWZ3yh+ern4l9dJpH/ipDSME0lCPF7kJwzKCOb5wC7lBEs2VARhTtWtEPcRR1iqFIsqhOmn8H/SPDQs07CujkrVs0kcBbANdsAesMAxqIJLUAcNgMEdeABP4Fm71x61F+113DqjTWa2wDdob58ErJ2u Z X t=13.5 fm/c

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 43 EVENT-BY-EVENT FLUCTUATIONS AT THE RHIC BES B. Schenke and C. Shen, in preparation • A good description of particle productions in AuAu collisions 0 250 500 750 dN/d¥ 0-6% (a) 6-15% (b) 15-25% (c) °6 °3 0 3 6 ¥ 0 200 400 dN/d¥ 25-35% (d) °6 °3 0 3 6 ¥ 35-45% (e) °6 °3 0 3 6 ¥ AuAu 200 GeV AuAu 62.4 GeV AuAu 19.6 GeV PHOBOS Event-averaged simulations Event-by-event with dynamical initialization

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 44 B. Schenke and C. Shen, in preparation • The event-by-event simulations give a better prediction for particle productions in d+Au collisions at RHIC BES Event-averaged simulations Event-by-event with dynamical initialization °6 °4 °2 0 2 4 6 ¥ 0 5 10 15 20 25 30 35 dNch/d¥ 0-5% dAu@ 200 GeV 0-5% dAu@ 62.4 GeV 0-10% dAu@ 39 GeV 0-20% dAu@ 19.6 GeV °6 °4 °2 0 2 4 6 ¥ 0 5 10 15 20 25 30 35 dNch/d¥ dAu @ BES 0-5% dAu @ 200 GeV 0-5% dAu @ 62.4 GeV 0-10% dAu @ 39 GeV 0-20% dAu @ 19.6 GeV 3D DESCRIPTION OF SMALL SYSTEMS AT THE RHIC BES

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 45 B. Schenke and C. Shen, in preparation • A good starting point to study longitudinal fluctuations in asymmetric systems at RHIC °6 °4 °2 0 2 4 6 ¥ 0 5 10 15 20 25 30 35 dNch/d¥ pAu dAu 3HeAu °4 °3 °2 °1 0 1 2 3 4 ¥ 0.00 0.02 0.04 0.06 0.08 0.10 v2 (¥) theory pAu 0-5% theory dAu 0-5% theory 3HeAu 0-5% PHENIX 0-5% pAu PHENIX 0-5% dAu PHENIX 0-5% 3HeAu 0-5% 200 GeV 200 GeV 3D DESCRIPTION OF SMALL SYSTEMS AT THE RHIC BES

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 46 CONSTRAINING LONGITUDINAL FLUCTUATIONS •Longitudinal flow decorrelation encodes the dynamical evolution of rapidity and thermal fluctuations Strong constraining power on longitudinal dynamics @ P. Bozek r2(⌘, ⌘ref ) = hV2(⌘) · V ⇤ 2 (⌘ref )i hV2( ⌘) · V ⇤ 2 (⌘ref )i AAACg3iclVFNTxsxEPUu5SttaaBHLhZRq6Qt6SYgCodIEVx6BKn5kLLpyuvMBguvd2XPIkWr/BF+Fjf+Dd5NVJGSC0+y9fxmnj2eCVMpDHrek+NuvNvc2t7Zrbz/8HHvU3X/oG+STHPo8UQmehgyA1Io6KFACcNUA4tDCYPw7qqID+5BG5GoPzhLYRyzqRKR4AytFFQfdNCmdR+Q/aDFHvgxw1sd5xqieYN2qB9pxnNfMjWVQPtBu0xuUJ9PEizOf7/V1xh9XRrmK87jN1mDas1reiXoa9JakhpZ4jqoPvqThGcxKOSSGTNqeSmOc6ZRcHtfxc8MpIzfsSmMLFUsBjPOyx7O6RerTGiUaLsU0lJ96chZbMwsDm1mUa35P1aI62KjDKPzcS5UmiEovngoyiTFhBYDoROhgaOcWcK4FrZWym+ZbTrasVXKJlwUOPv35dek3262TponN6e17uWyHTvkkByROmmRX6RLfpNr0iPcIc5X56fjuZvud7ftni5SXWfp+UxW4HaeAbL9wHQ= LHC RHIC A. Sakai, K. Murase and T. Hirano, arXiv:2003.13496 [nucl-th]

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 47 EARLY TIME DYNAMICS AT THE RHIC BES °3 °2 °1 0 1 2 3 ¥s 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 ø (fm) vs. °3 °2 °1 0 1 2 3 ¥s 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 ø (fm) p sNN = 19.6 GeV 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 AAACEnicdZDLSsNAFIYnXmu9RV26GSyCgoSkll4WQtGFrkoFe4EmlMl02g6dXJyZCCXkGdz4Km5cKOLWlTvfxkkvoKI/DPx85xzmnN8NGRXSND+1hcWl5ZXVzFp2fWNza1vf2W2KIOKYNHDAAt52kSCM+qQhqWSkHXKCPJeRlju6SOutO8IFDfwbOQ6J46GBT/sUI6lQVz+2xS2XsejaHpJD7sW1WpLAM2hVjKJ9MoeXpJl09ZxpVMrFfKEITcM0S1beSk2+VDgtQEuRVDkwU72rf9i9AEce8SVmSIiOZYbSiRGXFDOSZO1IkBDhERqQjrI+8ohw4slJCTxUpAf7AVfPl3BCv0/EyBNi7LmqM91R/K6l8K9aJ5L9shNTP4wk8fH0o37EoAxgmg/sUU6wZGNlEOZU7QrxEHGEpUoxq0KYXwr/N828YZmGdV3IVc9ncWTAPjgAR8ACJVAFV6AOGgCDe/AInsGL9qA9aa/a27R1QZvN7IEf0t6/APO0naI= 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

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 48 TRANSVERSE DYNAMICS WITH SOURCES • Fireball lives ~2 fm longer with dynamical initialization compared to the instantaneous setup • Hydrodynamic flow and its anisotropy develop slower with dynamical sources 0 2 4 6 8 10 12 ø (fm) 0.00 0.02 0.04 0.06 0.08 0.10 0.12 "p = hTxx ° Tyyi/hTxx + Tyyi 20-30% Au+Au @ 19.6 GeV dynamic instantaneous 0 2 4 6 8 10 12 14 ø (fm) 0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35 hTi (GeV) 0-5% Au+Au @ 19.6 GeV dynamic instantaneous C. Shen and B. Schenke, Nucl. Phys. A 982, 411-414 (2019)

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 49 DYNAMICAL VS INSTANTANEOUS INITIALIZATION C. Shen and B. Schenke, Nucl. Phys. A 982, 411-414 (2019) 0.0 0.5 1.0 1.5 2.0 2.5 3.0 pT (GeV) 10°3 10°2 10°1 100 101 102 103 dN/(2ºdypT dpT ) (GeV°2) º+ 0-5% Au+Au @ 19.6 GeV dynamical instantaneous STAR data 0.0 0.5 1.0 1.5 2.0 pT (GeV) 0.00 0.03 0.06 0.09 0.12 0.15 v2 (pT ) º+ 20-30% Au+Au @ 19.6 GeV dynamical instantaneous 0.0 0.5 1.0 1.5 2.0 2.5 3.0 pT (GeV) 10°3 10°2 10°1 100 101 102 103 º+ 0-5% Au+Au @ 19.6 GeV dynamical instantaneous STAR data • Dynamical initialization results steeper particle spectra and smaller v2(pT) 5-10% less radial and elliptic flow

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 50 DYNAMICAL INITIALIZATION EFFECT ON EM PROBES • Dynamical initialization results in large direct photon v2 at high pT EM probes show a large sensitivity to the early time dynamics Thermal + prompt photons C. Gale, S. Jeon, S. McDonald, J.F. Paquet and C. Shen, Nucl. Phys. A982 (2019) 767-770

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 51 C. Gale, S. Jeon, S. McDonald, J.F. Paquet and C. Shen, Nucl. Phys. A982 (2019) 767-770 EM TOMOGRAPHY AT RHIC BES ENERGIES Photons are unique soft penetrating probes to early time dynamics

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 52 ACCESSING NEW QGP TRANSPORT PROPERTY G. Denicol, C. Gale, S. Jeon, A. Monnai, B. Schenke and C. Shen, Phys. Rev. C98, 034916 (2018) L. Du and U. Heinz, arXiv:1906.11181 [nucl-th] • The charge diffusion current characterizes how conserved charges diffuse in and out of fluid cells • The is the QGP charge diffusion coefficient [matrix] qμ κ M. Li and C. Shen, Phys. Rev. C 98, 064908 (2018) =euµu⌫ (P+⇧) µ⌫+⇡µ⌫ Tµ⌫ Jµ =nuµ+qµ @µJµ = 0 P(e, n) + @µTµ⌫ = 0 ⇡µ⌫ ⇠ 2⌘rhµu⌫i ⇧ ⇠ ⇣@µuµ qµ ⇠ rµ µ T

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 53 ACCESSING NEW QGP TRANSPORT PROPERTY G. Denicol, C. Gale, S. Jeon, A. Monnai, B. Schenke and C. Shen, Phys. Rev. C98, 034916 (2018) L. Du and U. Heinz, arXiv:1906.11181 [nucl-th] • The net baryon diffusion current is driven by ; It transports more baryon charges to the mid-rapidity region ∇μ μ B T °5 °4 °3 °2 °1 0 1 2 3 4 5 y 0 10 20 30 40 50 dNp/dy ° dN ¯ p/dy no diÆusion with diÆusion CB = 0.6 BRAMHS 200 °5 °4 °3 °2 °1 0 1 2 3 4 5 y 0 10 20 30 40 50 dNp/dy ° dN ¯ p/dy no diÆusion with diÆusion CB = 0.6 STAR 19.6 M. Li and C. Shen, Phys. Rev. C 98, 064908 (2018)

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 54 G. Denicol, C. Gale, S. Jeon, A. Monnai, B. Schenke and C. Shen, Phys. Rev. C98, 034916 (2018) L. Du and U. Heinz, arXiv:1906.11181 [nucl-th] M. Li and C. Shen, Phys. Rev. C 98, 064908 (2018) °5 °4 °3 °2 °1 0 1 2 3 4 5 y 0 10 20 30 40 50 dNp/dy ° dN ¯ p/dy no diÆusion with diÆusion CB = 0.6 BRAMHS 200 °5 °4 °3 °2 °1 0 1 2 3 4 5 y 0 10 20 30 40 50 dNp/dy ° dN ¯ p/dy no diÆusion with diÆusion CB = 0.6 STAR 19.6 •Net charge diffusion driven by transports more charges to the mid- rapidity region rµ µq T AAACA3icbZDLSsNAFIYnXmu9Rd3pZrAIrkLSaGt3RTcuK/QGTS2T6aQdOpnEmYlQQsGNr+LGhSJufQl3vo3TtIi3HwY+/nMOZ87vx4xKZdsfxsLi0vLKam4tv76xubVt7uw2ZZQITBo4YpFo+0gSRjlpKKoYaceCoNBnpOWPLqb11i0Rkka8rsYx6YZowGlAMVLa6pn7Hkc+Q9demEAvEAinmno3k7Q+6ZkF26q4ZadShhkU3dIcnFPoWHamApir1jPfvX6Ek5BwhRmSsuPYseqmSCiKGZnkvUSSGOERGpCORo5CIrtpdsMEHmmnD4NI6McVzNzvEykKpRyHvu4MkRrK37Wp+V+tk6jgrJtSHieKcDxbFCQMqghOA4F9KghWbKwBYUH1XyEeIp2E0rHlZyFMVfo6+S80i5bjWu7VSaF6Po8jBw7AITgGDiiDKrgENdAAGNyBB/AEno1749F4MV5nrQvGfGYP/JDx9gkeJZij ACCESSING NEW QGP TRANSPORT PROPERTY rµ µq T AAACA3icbZDLSsNAFIYnXmu9Rd3pZrAIrkLSaGt3RTcuK/QGTS2T6aQdOpnEmYlQQsGNr+LGhSJufQl3vo3TtIi3HwY+/nMOZ87vx4xKZdsfxsLi0vLKam4tv76xubVt7uw2ZZQITBo4YpFo+0gSRjlpKKoYaceCoNBnpOWPLqb11i0Rkka8rsYx6YZowGlAMVLa6pn7Hkc+Q9demEAvEAinmno3k7Q+6ZkF26q4ZadShhkU3dIcnFPoWHamApir1jPfvX6Ek5BwhRmSsuPYseqmSCiKGZnkvUSSGOERGpCORo5CIrtpdsMEHmmnD4NI6McVzNzvEykKpRyHvu4MkRrK37Wp+V+tk6jgrJtSHieKcDxbFCQMqghOA4F9KghWbKwBYUH1XyEeIp2E0rHlZyFMVfo6+S80i5bjWu7VSaF6Po8jBw7AITgGDiiDKrgENdAAGNyBB/AEno1749F4MV5nrQvGfGYP/JDx9gkeJZij °5 °4 °3 °2 °1 0 1 2 3 4 5 y 0 10 20 30 40 50 dNp/dy ° dN ¯ p/dy no diÆusion with diÆusion CB = 0.6 BRAMHS 200 Not enough in high energy collisions

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 55 •Allowing the initial baryon charges to fluctuate to string junctions improves description at high collision energies Interplay between baryon diffusion and initial fluctuations D. Kharzeev, Phys. Lett. B 378, 238 (1996) °4 °2 0 2 4 y 0 20 40 60 80 dNp/dy ° dN ¯ p/dy 0-5% AuAu AuAu 200 GeV AuAu 62.4 GeV AuAu 19.6 GeV AuAu 7.7 GeV STAR BRAMHS °4 °2 0 2 4 y 0 5 10 15 20 25 30 35 dNp/dy ° dN ¯ p/dy 0-5% AuAu@200 GeV string end string junction STAR BRAMHS C. Shen and B. Schenke, in preparation INITIAL STATE BARYON STOPPING

Chun Shen (WSU/RBRC) UH/UIUC Journal Club 56 SUMMARY • Relativistic heavy-ion collisions over 3 orders of magnitude in collision energy map out the phase structure of hot QCD matter • Full 3D hybrid framework starts to quantitatively describe bulk observables at the RHIC BES program Elucidating the initial baryon stopping, charge diffusion, and collectivity of QGP in a baryon rich environment Build connections with neutron star/black hole mergers First principle inputs from lattice QCD Search for a critical point and the first-order phase transition Consistent 3D dynamical descriptions of pp, pA, and AA collisions