Predictions for 5.02A TeV Pb+Pb Collisions from A Multi-Phase Transport Model

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Predictions for 5.02A TeV Pb+Pb Collisions from A Multi-Phase Transport Model Zi-Wei Lin East Carolina University, Greenville, NC Results are mainly based on G.L. Ma & ZWL, Phys Rev C 93 (2016) /arxiv:1601.08160

A Multi-Phase Transport Model (AMPT) aims to provide a comprehensive kinetic description of essential stages of high energy heavy ion collisions A+B Initial conditions Parton Interactions Hadronization Hadron Cascade Long paper: ZWL, Ko, Li, Zhang and Pal, PRC 72 (2005); source codes at the ECU website http://myweb.ecu.edu/linz/ampt/ Final particle spectra

Structure of the String Melting version of AMPT A+B HIJING1.0: minijet partons (hard), excited strings (soft), spectator nucleons Generate parton space-time Partons freeze out ZPC (elastic parton cascade) Hadronization (Quark Coalescence) Strings melt to q & qbar via intermediate hadrons Extended ART (hadron cascade) Final particle spectra Hadrons freeze out (at a global cut-off time); then strong-decay all remaining resonances

One Au+Au event at 200AGeV from String Melting AMPT 60fm-long box Side view: Beam axes Animation is available at the AMPT webpage

One Au+Au event at 200AGeV from String Melting AMPT at time=5 fm/c 60fm-long box Side view: Beam axes

AMPT webpage at http://myweb.ecu.edu/linz/ampt/

String Melting AMPT at 200A GeV and 2.76A TeV: model can reasonably reproduce bulk π & K data at low P T dn/dy of π & K: ZWL, PRC 90 (2014)

String Melting AMPT at 200A GeV and 2.76A TeV p T -spectra of π & K (in central collisions): ZWL, PRC 90 (2014)

Simplified picture of elliptic flow v 2 due to azimuthal anisotropy in space: String Melting AMPT at 200A GeV and 2.76A TeV ZWL, PRC 90 (2014) Elliptic flow v 2 of π & K (in mid-central collisions): We then use the same model parameters for 2.76TeV Pb+Pb collisions to predict 5TeV Pb+Pb collisions: G.L. Ma & ZWL, PRC 93 (2016)

AMPT predictions for 5TeV Pb+Pb: dn ch /dη Although we had these dn/dη results before the announcement of the ALICE 5.02 TeV data arxiv:1512.06104, we did not post these before the data. So the 5TeV dn/dη results at η~0 are strictly speaking not predictions. The full dn/dη curves are still predictions. G.L. Ma & ZWL, PRC 93 (2016) /arxiv:1601.08160 0-5% centrality 20-30%

AMPT predictions for 5TeV Pb+Pb: charged particle flows v 2,v 3,v 4 ALICE v 2 data at 5.02TeV announced later in arxiv:1602.01119

AMPT predictions for 5TeV Pb+Pb: charged particle v 2 (η) ALICE v 2 (η) data at 2.76TeV announced later in arxiv:1605.02035

AMPT predictions for 5TeV Pb+Pb: longitudinal correlations The initial spatial geometry including the event plane depends on η Pb nucleus=208 nucleons but also has longitudinal correlations. Lorentz contraction projects the nuclear sphere on the transverse plane Elementary collisions deposit energy at the transverse location of the nucleons Thus the initial density profile is typically uniform longitudinally, but Strings with a in AMPT Boost-invariant hydrodynamics, bumpy (before transverse melting profile the strings to partons) Gelis 1110.1544 from Ollitrault, Quark Matter 2015 25 This longitudinal correlation comes naturally in string melting AMPT, since each wounded nucleon (string) can produce multiple initial partons that have almost the same transverse position but a range of different η values.

AMPT predictions for 5TeV Pb+Pb: longitudinal correlations The initial spatial geometry including the event plane depends on η but also has longitudinal correlations. The azimuthal anisotropies v n then has correlations over a finite η range. Charged particle r 2 (η a, η b ) Ma & ZWL, PRC93 (2016) For results of AMPT (as initial condition) +hydro, see Pang et al. PRC91(2015) & EJPA52 (2016).

Summary AMPT serves as a comprehensive model for heavy ion collisions: Event-by-event from initial condition to final observables Can address non-equilibrium dynamics Self-consistent chemical and kinetic freeze-out It is a test-bed of different ideas & can lead to new discoveries: Example: the discovery of the triangular flow v 3 Example: v 2 & v 3 may be dominated by anisotropic escape instead of hydrodynamics flow, due to low/modest opacity Significant further developments are needed: improve dynamical quark coalescence / parton recombination; include gluons and inelastic parton reactions; high P T (with radiation energy loss);