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Event-by-Event Fluctuations of Net-Baryon Distribution and Higher Order Cumulants ZHOU You , LIU Feng Institute Of Particle Physics (IOPP) HuaZhong Normal University (HZNU) HuaZhong Normal University IWND09, August 22~25, Shanghai 1 outline • Motivation • Some definitions and MC data • Results of centrality dependence, transverse momentum dependence, rapidity dependence, & energy dependence, of fluctuations of Net-Baryon distribution and higher order cumulants • Summary and Outlook HuaZhong Normal University IWND09, August 22~25, Shanghai 2 motivation QCD Phase Diagram RHIC beam energy scan program : Locate the QCD critical point. Figure 1 Draw the QCD phase boundary. CP STAR Beam User Request ★ Mapping the QCD phase diagram ★ Searching the Critical Point HuaZhong Normal University Key measurements: (1) PID hadron spectra, ratios, v2 … (2) Fluctuations: - Net-p Kurtosis - K/ - <pT>, <N> … JY Chen for STAR -CPOD2009 IWND09, August 22~25, Shanghai 3 motivation baryon number fluctuation is a highlight in heavy ion physics and studying the event-byevent fluctuations of observable provide useful tools to research the critical point arXiv: 0606047 arXiv: 0805.0236 arXiv: 0809.0685 arXiv: 0903.2911 Phys. Rev. D 79, 074505 (2009) nayak(STAR Collaboration)@QM2009 M. A. Stephanov, PRL 102, 032301 (2009) ... "non-Gaussian moments (cumulants) of fluctuations of experimental observable are very sensitive to the proximity of the critical point, as measured by the magnitude of the correlation length " at the Critical Point 2 2 2nd Order Cumulant: (N ) ~ 4th Order Cumulant: ()4 3 ( N )2 2 7 is Correlation length is a measure of the range over which fluctuations in one region of space are correlated with those in another • Sensitive to long range correlations • Shows large non-monotonic behaviour as a function of T 4th Order Cumulant is more sensitive than 2nd Order Cumulant to study the CP HuaZhong Normal University IWND09, August 22~25, Shanghai 4 motivation M.Cheng et al. arXiv: 0811.1006 v3 [hep-lat] M.Cheng et al.Phys. Rev. D 79, 074505 (2009) Figure 2 Figure 3 in all cases the quadratic(2nd order) fluctuations rise rapidly in the transition region and approach to SB limit where the quartic(4th order) fluctuations show a maximum. This maximum is most pronounced for the baryon number fluctuations. the value 4 / 2 for net-baryon is about 1.0 when T< 200MeV which consist with HRG. It is closed to SB limit when T >200MeV ☞ The measurement of higher order cumulants of net-baryon distribution and its variations will provide the connection between experimental observable and Lattice Gauge Theory calculations. HuaZhong Normal University IWND09, August 22~25, Shanghai 5 analysis ☞ C2 ( N ) 2 N 2 N 2 2 ☞ ☞ • MC data we used: 2nd Order Cumulant: is Standard deviation ( N )3 ( N )4 4 3 a measure of the peakedness of the distribution for a Gaussian distribution, the value of skewness and kurtosis is 0 ☞ R4, 2 C4 C2 Events Events Events Events 3 a measure of the symmetry of a distribution ☞ Kurtosis all for Au+Au collision RQMD v2.4: 9.2 GeV ~4M 12.3GeV ~1M 17.3GeV ~1M 20 GeV ~3M 4th Order Cumulant: C4 ( N ) 4 3 ( N ) 2 2 Skewness ☞ HuaZhong Normal University UrQMD v2.3: 9.2 GeV ~16M Events AMPT v2.11: 9.2 GeV(3mb) Default ~2M Events String Melting ~8M Events IWND09, August 22~25, Shanghai 6 centrality dependence for Net-Baryon Au+Au S NN 9.2GeV RQMD v2.4 0< pT <1.0 (GeV/c) |Y|<0.5 Figure 4 from peripheral to central collisions: • Mean values <NB>, C2 increase smoothly • Skewness and Kurtosis: decreasing • C4 and R4,2 decreases rapidly in central collision HuaZhong Normal University IWND09, August 22~25, Shanghai 7 transverse momentum dependence Net-Baryon pT distribution for net-baryon Figure 9 Figure 10 • The results of different pT do not take effect distinctly although the value are not the same. HuaZhong Normal University IWND09, August 22~25, Shanghai 8 rapidity dependence Net-Baryon rapidity distribution Figure 12 Figure 13 ☞ rapidity window ① |Y|<0.5 ② |Y|<1.0 different rapidity also do not play an active role HuaZhong Normal University IWND09, August 22~25, Shanghai 9 rapidity dependence ☞ rapidity region Net-Baryon 0< pT <1.0(GeV/c) 0.5< |Y| <1.0 Figure 15 Figure 14 they all have similar trends although a diverge happened in central collision for C4、R4,2 HuaZhong Normal University IWND09, August 22~25, Shanghai 10 energy dependence of C4 Net-Baryon Figure 6 Figure 5 the right panel shows at 9.2, 12.3, 17.3, 20 GeV, C4 exhibit unlike behaviour. But we can get non-monotonic behaviour at all time. HuaZhong Normal University IWND09, August. 22~25, Shanghai 11 energy dependence of KB Net-Baryon Figure 7 Figure 8 the left panel shows energy dependence of KB, in central collision, the trend are seen the same the right panel shows at 9.2, 12.3, 17.3, 20 GeV, KB exhibit similar behaviour. HuaZhong Normal University IWND09, August. 22~25, Shanghai 12 MC model difference UrQMD for Net-Baryon Figure 16 other MC models are used to check our results HuaZhong Normal University IWND09, August. 22~25, Shanghai 13 MC model difference AMPT for Net-Baryon Figure 17 we can find the trend of UrQMD and AMPT are similar to those of RQMD HuaZhong Normal University IWND09, August 22~25, Shanghai 14 Summary and Outlook • We have presented a study of mean value <NB>, variance C2, skewness, kurtosis(KB), C4 and R4,2 of eventby-event net-baryon distribution. The trend of centrality dependence of different pT and Y window are similar Calculations from UrQMD and AMPT model also support our conclusion • This work present baseline predictions of Net-Baryon distribution and higher order cumulants, it will help to understand the expectations from experiment results for the forthcoming RHIC Beam Energy Scan Program. • Next to do: 1 Centrality dependence Net-Baryon distribution at high Energy 2 Net-Charge Kurtosis HuaZhong Normal University IWND09, August 22~25, Shanghai 15 Thanks for your attention also thanks to the Organizer of IWND2009 HuaZhong Normal University IWND09, August 22~25, Shanghai 16 backup HuaZhong Normal University IWND09, August 22~25, Shanghai 17 analysis ① observable LGT T Critical Point centrality dependence Tcentral > Tperipheral observable T energy dependence ThighEnergy > TlowEnergy ② how does the different cut effect the results of all observable transverse momentum dependence HuaZhong Normal University rapidity dependence IWND09, August 22~25, Shanghai 18 • The quadratic fluctuations of light and strange quark number versus temperature (upper figure) and the ratio of s and •u quark fluctuations on T 3 3 24 lattices of size 16 × 4 and ×6,respectively. h e q 22~25, Shanghai HuaZhong Normal University IWND09, August 163 243 19 transverse momentum dependence Net-Baryon ☞ PT region 0.0 < PT<0.5 0.5 < PT <1.0 1.0 < PT <1.5 1.5 < PT <2.0 Figure 11 0.5<PT<1.0(GeV/c) mean、C2、skewness、KB have the similar trend C4 and R4,2 seems different in four PT regions HuaZhong Normal University IWND09, August 22~25, Shanghai 20 arXiv:0903.2911v2 [hep-ph] The fluctuations of net-baryon number in a subsystem are of the order of the root of the average netbaryon number in this subsystem. HuaZhong Normal University