Elliptic flow of meson in Pb-Pb Paola Pagano 09/12/2009 Paola Pagano Università di Salerno & INFN 1 Elliptic flow The flow is a collective motion of the particles produced in the ultrarelativistic nuclear reaction. A non central collision produces an anisotropic flow in the transverse plane spectators z participants spectators y x The anisotropic transverse flow, i.e. elliptic flow, springs from the initial azimuthal asymmetry of the interaction region 09/12/2009 Paola Pagano Università di Salerno & INFN 2 Elliptic flow It has origin from the anisotropic nature of the overlap region in the plane x-y with impact parameter b>0 b=0 The secondary interaction of particles converts the initial spatial anisotropy in an observed momentum anisotropy in the final state 09/12/2009 Paola Pagano Università di Salerno & INFN 3 Elliptic Flow To measure the elliptic flow, we need first reaction to distribution the Then the plane. coefficients expansion estimate of of of the the y 2 Fourier azimuthal particles with x respect to the reaction plane are evaluated. Poskanzer and Voloshin, Phys. Rev. C58, 1998 N0 dN 1 2v1 cos( 2 ) 2v2 cos2 2 .... d ( 2 ) 2 Elliptic flow coefficient 09/12/2009 Paola Pagano Università di Salerno & INFN 4 Elliptic flow measurement: recent results at RHIC A scaling of the elliptic flow parameter v2 with the number of quarks is observed To describe the observed scaling, two different models have been used: •Quark recombination models • Hadronic transport models. 2007 09/12/2009 In the context of both models, the observed v2 values seem to indicate that elliptic flow is built up prior to hadronization, in the partonic phase. Paola Pagano Università di Salerno & INFN 5 meson’s elliptic flow measurement : recent results at RHIC (I) 2007 v2 of meson increases with the eccentricity of the central region of overlap (i.e. the reduction of the centrality) 09/12/2009 Paola Pagano Università di Salerno & INFN 6 meson’s elliptic flow measurement: recent results at RHIC (II) 2007 NQ-scaling fit -mesons are produced via coalescence of seemingly thermalized quarks in central Au+Au collisions. phi meson NQ = 2.3 ± 0.4 This observation implies that hot and dense matter with partonic collectivity has been formed at RHIC 09/12/2009 Paola Pagano Università di Salerno & INFN 7 How can we perform this measurement in ALICE? Mass invariant method 1) Mass invariant histogram for phi meson 2) Estimation of Signal and Background: fit with Breit-Wigner + polynomial 3) Estimation of reaction plane angle for each event: wi sin( 2i ) 1 1 2 tan 2 wi cos( 2i ) 09/12/2009 Paola Pagano Università di Salerno & INFN wi e i for the l’ith particle of a given event 8 How can we perform this measurement in ALICE? Mass invariant method (cont’d) 4) Estimate of the opening angle for all K+K- pairs for each event 5) Histogram of v2(minv)= <cos2(KK-2)> 6) Fit of the last histogram with the function: v2(minv) = a(minv)v2S+[1-a(minv)]v2B(minv) where v2(minv) = <cos2(KK-2)> v2S is the v2 we are looking for v2B is the v2 of combinatorial background a(minv) = N(minv) / NK+ K_ (minv) 09/12/2009 Paola Pagano Università di Salerno & INFN 9 Status of the analysis • The analysis tools are ready. • We are still producing a sufficient number of events Estimation: approximately 106 events. • Two Productions: - one official, managed by the collaboration, for the production of the background, now I’m generating the signal - one private, containing only the generated particles without recostruction-> ongoing on the Salerno computer cluster • The time and space needed to perform this analysis, make essential the use of the world computing Grid facility. • Here we show some preliminary results for the estimation of: - reaction plane angle - v2 for all particles 09/12/2009 Paola Pagano Università di Salerno & INFN 10 Reaction Plane Angle estimation: checking the algorithm Generated Particles Reconstructed Particles wi sin( 2i ) 1 1 2 tan 2 wi cos( 2i ) 09/12/2009 Paola Pagano Università di Salerno & INFN 11 v2 estimation: checking the generator After the determination of reaction plane angle Ψ2 , it’s possible to build a global distribution dN/d(φ-Ψ2) using events with same multiplicity and centrality. This distribution can be interpolated with the function: dN/dφ = cost.(1/2π) + 2 v2 cos2(φ-Ψ2) v2: 0.02794 ± 0.0011 Generated Particles v2: 0.03163 ± 0.0011 φ-Ψ2 (degree) Reconstructed Particles 21/12/2015 12 φ-Ψ2 (degree) The End 09/12/2009 Paola Pagano Università di Salerno & INFN 13 Back up Metodo della matrice di sfericità trasversa (I) i cos i sin cos i i i sin i cos i S11 S sin i i 12 i S12 S 22 • Diagonalizzazione della matrice di sfericità trasversa S11 S12 S12 S 22 0 Metodo della matrice di sfericità trasversa (II) S11 S 22 ( S11 S 22 ) 4S 1, 2 2 1 2 Il rapporto è proporzionale a v2 1 2 2 2 12 Dagli autovettori si ricava l’angolo del piano di reazione 2 : S12 21 ATan2 S11 1