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Bedanga Mohanty VECC, Kolkata mesons in High Energy Nuclear Collisions Outline meson in High Energy Collisions Review of existing results Strangeness Enhancement Partonic Collectivity Recombination and hints of Thermalization Probing QCD Phase Boundary : v2 measurement Thanks to Nu Xu, Jinhui Chen, Zhangbu Xu, Huan Huang, Guoliang Ma and STAR for discussions QGP Meet 2008 : Bedanga Mohanty
First seen in bubble chamber experiments at Brookhaven in 1962 in the reactions K- + p L + K+K K- + p L + K++K- Mass 1020 MeV, G<<20 MeV Quantum numbers JPC = 1-- mesons - Discovery STAR @ RHIC, BNL High signal for the decay to KK, at the edge of the kinematically allowed region, rp decay suppressed STAR : QM2008 QGP Meet 2008 : Bedanga Mohanty
mesons QGP Meet 2008 : Bedanga Mohanty
Golden ratio meson in high energy collisions Remark A goldentool which can be used to address various aspect of heavy-ion collisions Next : meson and Strangeness Enhancement QGP Meet 2008 : Bedanga Mohanty
P. Koch, B. Muller,J. Rafelski Phys. Rep. 88 (1982) 331 Phys. Rev. Lett. 48 (1982) 1066 Phys. Rep. 142 (1986) 167 Canonical Effect in p+p collisions : Quantum Numbers exactly conserved J. Cleymans, A. Muronga, K. Redlich, A. Tounsi, et al. Suppression causes : -Strangeness ordering -Beam energy dependence Phys. Lett. B. 388 (1996) 401 Phys. Rev. C 58 (1997) 2747 Phys. Rev. C 57 (1998) 3319 Phys. Lett. B. 486 (2000) 61 Eur. Phys. J. C 24 (2002) 589 hep-ph/0111159 QGP scenario : Strangeness Enhancement Copious production of s and sbar pairs Strangeness enhancement relative to p+p collisions Stronger effect for multi-strange hadrons and increases with strangeness content QGP Meet 2008 : Bedanga Mohanty
arXiv:0810.4979 mesons and Strangeness Enhancement Strangeness enhancement observed -- Dense partonic medium formation in A+A ? -- Canonical suppression in p+p ? Statistical model predictions -- Enhancement increases with strange-quark content -- Enhancement higher for lower beam energy at RHIC energies: -- Not canonically suppressed -- Does not follow number of strange-quark ordering -- Enhancement(62.4) < Enhancement(200) STAR Preliminary • enhancement between K-() and ? STAR :arXiv:0804.4363 : J.Phys.G35:044031,2008 Possible Issues : If formed by KK coalescence can be subjected to Canonical suppression. Is production OZI suppressed in p+p collisions ? QGP Meet 2008 : Bedanga Mohanty
Production from KK Coalescence Naively from KK Coalescence If formed by KK Coalescence -- K- ratio will change with collision centrality/Beam energy/System size -- Width of rapidity distribution : 1/ ~ 1/K- + 1/K+ --- Inverse Slope of transverse momentum distribution : T~ 2 TK --- and K v2 measurements (discussed later) --- Constraints due to the spin quantum number (K are spin 0 and is spin 1) production not from KK coalescence at RHIC energies Observed strangenessenhancement not due to Canonical suppression effects RMS rapidity dist. STAR : Phys. Rev. Lett. 99 (2007) 112301 Phys. Lett. B 612 (2005) 181 arXiv:0809.4737 NA49 : arXiv:0806.1937 Phys. Rev. Lett. 96 (2005) 052301
Violations of OZI rule observed in p+p collisions. - u d Phys. Lett. B 59 (1975) 88 arXiv: nucl-th/9907059 K - s or c s d for J/y 0 R()=tan2()= 4.2 X10-3: deviation from ideal mixing angle f s or c d s Phys. Lett. B 60 (1976) 371 Phys. Lett. B 353 (1995) 319 Phys. Lett. B 592 (2004) 1 u K+ d + OZI suppressed Not OZI suppressed Phys. Lett. 5 (1963) 165 CERN Report Nos. TH-401 and TH-412 (1964) (unpublished) Prog. Theor. Phys. 35 (1966) 1061 Okubo Zweig Iizuka Suppression of Suppression of interaction with nucleons, non-strange mesons and resonances At high colliding energies at RHIC -- OZI suppression could be lifted Observed enhancement not due to OZI suppression in p+p collisions
Golden ratio meson in high energy collisions Remark A goldentool which can be used to address various aspect of heavy-ion collisions Strangeness enhancement in heavy-ion collisions at RHIC is due to formation of a dense partonic medium and not alone due to Canonical Suppression effects STAR Preliminary meson Strangeness Enhancement Next meson - Partonic Collectivity, Recombination and Thermalization QGP Meet 2008 : Bedanga Mohanty
y 2v2 dN/df dN/df 0 2p 0 f 2p Collectivity Pressure gradiant Initial spatial anisotropy x INPUT Spatial Anisotropy Interaction among produced particles OUTPUT Momentum Anisotropy QGP Meet 2008 : Bedanga Mohanty
STAR : Phys. Rev. Lett. 99 (2007) 112301 PHENIX : Phys. Rev. Lett. 99 (2007) 052301 Partonic collectivity at RHIC Substantial v2 measured for mesons v2 similar to other mesons Constituent Quark Scaling observed Reflects partonic collectivity : Heavier s quarks flows as lighter u and d quarks To further strengthen the idea of partonic collectivity --not formed from KK coalescence (already discussed) -- likely decouples early in interactions and does not participate strongly in hadronic interactions QGP Meet 2008 : Bedanga Mohanty
Au+Au ~ 3 ~ 3.5 frezee-out at RHIC just after Tc from Lattice QCD ~ 2.6 ~ 4 ~ 2.1 Van Hecke, Sorge, Xu (98) No decay b=2.0fm arXiv:nucl-th/0509061 STAR : Nucl. Phys. A 757 (2005) 102 arXiv:nucl-th/0606044 STAR : Phys. Lett. B 612 (2005) 181 possibly decouples early ~ 10 mb <pT> is almost independent of centrality unlike anti-protons Indicates possibly decouples early in the interaction decouples from the system early at RHIC energies
STAR preliminary Au+Au@200GeV Cu+Cu@200GeV Recombination and Hints of Thermalization Clear change in spectral shape -- Exponential (~thermal) for central collisions -- Power law type (~ hard process) at high pT in peripheral collisions Monotonic rise of ratio at low pT -- Good agreement with models based on and production by thermal s-quark coalescence STAR : Phys. Rev. Lett. 99 (2007) 112301 arXiv: nucl-th:0406072 arXiv:0809.4737 QGP Meet 2008 : Bedanga Mohanty
Golden ratio meson in high energy collisions Remark A goldentool which can be used to address various aspect of heavy-ion collisions Strangeness enhancement in heavy-ion collisions at RHIC is due to formation of dense partonic medium and not alone due to Canonical Suppression effects STAR Preliminary meson Strangeness Enhancement meson : Partonic Collectivity and Thermalization The collectivity observed in heavy-ion collisions at RHIC is due to partonic interactions. Hints of formation of some kind of thermalized (partial?) system Next meson as a probe for QCD phase boundary QGP Meet 2008 : Bedanga Mohanty
: Probe QCD phase diagram • Supporting observations from previous • discussions - • -- Primordial production ~ 100% • - Decouples early from the system ~ TC • - Not formed from KK Coalescence • - Hadronic interactions small/OZI suppressed • -- ss structure and Strangeness enhancement • due to dense partonic matter formation • -- Substantial v2 observed in Au+Au 200 GeV • -- NCQ Scaling NA49 Key observable : v2 of meson RHIC data suggests - collectivity observed in due to partonic interactions Absence/reduction of collectivity and NCQ scaling of could indicate system in Hadronic phase QGP Meet 2008 : Bedanga Mohanty
Wu Kejun v2 expectation from AMPT Default setting, ~ 10 mb No NCQ Scaling observed Large v2 ofcould bedue to KK contributions Partonic Coalescence NCQ scaling observed QGP Meet 2008 : Bedanga Mohanty
Golden ratio meson in high energy collisions Remark A goldentool which can be used to address various aspect of heavy-ion collisions Strangeness enhancement in heavy-ion collisions at RHIC is due to formation of a dense partonic medium and not alone due to Canonical Suppression effects meson Strangeness Enhancement meson : Partonic Collectivity, Recombination and Thermalization The collectivity observed in heavy-ion collisions at RHIC is due partonic interactions. Hints of formation of some kind of thermalized (partial?) system meson as a probe for QCD phase boundary Large Collectivity and Number of Constituent Quark Scaling of v2 -- clear indication matter went through partonic phase QGP Meet 2008 : Bedanga Mohanty
mesons : Summary QGP Meet 2008 : Bedanga Mohanty
Highlights STAR Preliminary Strangeness enhancement at RHIC Due to formation of dense partonic medium Collectivity at RHIC Developed due to partonic interactions QCD phase boundary Small v2 andabsence of NCQ scaling - Hadronic phase Large v2 and NCQ scaling - Partonic phase QGP Meet 2008 : Bedanga Mohanty
b a De Divina Proportione Normal Human Heart Beats in rhythm • p-p+p0is suppressed compared to K-K+ (which is actually kinematically suppressed) "Feynman taught me that in strong interaction physics everything that can possibly happen does, and with maximum strength,only conservation laws suppress reactions. Here was a reaction that was allowed but did not proceed.” -- Zweig = 1.61803.. The Golden Ratio is a universal law : in which is contained the ground-principle of all formative striving for beauty and completeness in the realms of both nature and art, and which permeates, as a paramount spiritual ideal, all structures, forms and proportions, whether cosmic or individual, organic or inorganic, acoustic or optical; which finds its fullest realization, however, in the human form. -- Adolf Zeising QGP Meet 2008 : Bedanga Mohanty
Back up QGP Meet 2008 : Bedanga Mohanty
Hadronic matter Small v2 - Support from Models J.Phys.G32:1121-1130,2006 URQMD partonic Supporting arguments for small v2 for hadronic matter -- v2 large only if there is partonic interactions Largev2 from KK coalescence, but production unlikely from KK coalescence Hence small v2 expected if matter went through hadronic phase only QGP Meet 2008 : Bedanga Mohanty
STAR : Phys. Rev. Lett. 99 (2007) 112301 High pT probing partonic matter STAR Preliminary STAR : arXiv:0809.4737 Observations : Suppression in 200 GeV Au+Au collisions No suppression in 200 GeV d+Au collisions Interpretation : Dense medium formed in 200 GeV Au+Au collisions Turn-off of suppression may indicate hadronic matter Advantage over other hadrons : Production likely via parton coalescence Understand difference in quark vs. gluon energy loss arXiv:0705.0953 QGP Meet 2008 : Bedanga Mohanty