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Centrality Dependence of Freeze-out Parameters From the Beam Energy Scan at STAR

Centrality Dependence of Freeze-out Parameters From the Beam Energy Scan at STAR. Sabita Das (for the STAR collaboration) Institute of Physics, Bhubaneswar, India. Outline. Motivation Introduction - Chemical freeze-out - Kinetic freeze-out Experimental set-up

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Centrality Dependence of Freeze-out Parameters From the Beam Energy Scan at STAR

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  1. Centrality Dependence of Freeze-out Parameters From the Beam Energy Scan at STAR Sabita Das (for the STAR collaboration) Institute of Physics, Bhubaneswar, India Quark Matter 2012, Washington D.C, USA Sabita Das

  2. Outline • Motivation • Introduction - Chemical freeze-out - Kinetic freeze-out • Experimental set-up • Particle Identification method • Results on freeze-out parameters • Summary Quark Matter 2012, Washington D.C, USA Sabita Das

  3. Motivation • The main goals of RHIC BES • program - To map the QCD phase diagram - To search the possible QCD phase boundary - To search the possible QCD critical point • The STAR data from BES are used • to extract the freeze-out parameters • T, mB and <b> from identified particle • spectra and ratios QCD Phase Diagram STAR BES proposal: arXiv:1007.2613 Quark Matter 2012, Washington D.C, USA Sabita Das

  4. Introduction Chemical Freeze-out : Inelastic collision ceases Particle ratios get fixed ★THERMUS : Statistical thermal model Ensemble used – Grand Canonical and Strangeness Canonical For Grand Canonical: Quantum numbers (B, S, Q) conserved on average To consider incomplete strangeness equilibration: For Strangeness Canonical: Strangeness quantum number (S) conserved exactly Extracted thermodynamic quantities: Tch,μB, μsandγS • Thermus, S. Wheaton & Cleymans, Comput. Phys. Commun. 180: 84-106, 2009. Quark Matter 2012, Washington D.C, USA Sabita Das

  5. Introduction Kinetic Freeze-out : Elastic collision ceases Transverse momentum spectra get fixed Blast Wave : Hydrodynamic inspired model E. Schnedermann et al., Phys. Rev. C 48, 2462 (1993) Particle spectra are fitted simultaneously Extracted thermodynamic quantities: Tkinand<β> Quark Matter 2012, Washington D.C, USA Sabita Das

  6. TheSolenoidTrackerAtRHIC (STAR) Full azimuthal particle identification. TOF TPC Data (2010): Au+Au 39GeV, 11.5 GeV and 7.7 GeV. Particles used : π, K, p, Λ, Ξ and K0S Quark Matter 2012, Washington D.C, USA Sabita Das

  7. Particle Identification TPC+TOF TPC STAR Preliminary STAR Preliminary STAR Preliminary Counts Counts STAR Preliminary p = momentum, t = time-of-flight c = velocity of light, L = path length zπ m2 (GeV2/c4) arXiv:1201.4203v1 Quark Matter 2012, Washington D.C, USA Sabita Das

  8. Particle Spectra STAR Preliminary STAR Preliminary STAR Preliminary arXiv:1201.4203v1 arXiv:1203.5183 STAR Preliminary STAR Preliminary STAR Preliminary Quark Matter 2012, Washington D.C, USA Sabita Das

  9. Chemical Freeze-out STAR Preliminary STAR Preliminary • Particles used : • π, K, p, Λ , Ξ • and K0s • Ensemble used: • Grand Canonical • Fit parameters: • Tch,μB,,μs andγS • (strangeness • saturation factor) STAR Preliminary STAR Preliminary Quark Matter 2012, Washington D.C, USA Sabita Das

  10. Chemical Freeze-out Au+Au 200 GeV : Phys. Rev. C 83 (2011) 24901 • Particles used in the fit: π, K, p, Λ , Ξ andK0s • Chemical freeze-out temperature increases with increase in collision energy. • Baryon chemical potential decreases with increase in collision energy. Quark Matter 2012, Washington D.C, USA Sabita Das

  11. Chemical Freeze-out Au+Au 200 GeV : Phys. Rev. C 83 (2011) 24901 • Particles used in the fit : π, K, p, Λ , Ξ and K0s • Strangeness chemical potential decreases with increase in collision energy • Strangeness saturation factor increases from peripheral to central collisions for • all energies Quark Matter 2012, Washington D.C, USA Sabita Das

  12. Chemical Freeze-out: Tch vs. mB • Particles used : • π, K, p, Λ , Ξ • andK0s • Ensemble used: • Grand Canonical • and Strangeness • Canonical • Fit parameters: • Tch,μB,,μs andγS • (strangeness • saturation factor) Andronic: NPA 834 (2010) 237 Cleymans: PRC 73 (2006) 034905 Au+Au 200 GeV : Phys. Rev. C 83 (2011) 24901 STAR Preliminary • We observe a centrality dependence of • chemical freeze-out parameters (Tch,mB) • at lower energies. • For peripheral collisions: Tch (SCE) > Tch (GCE) Quark Matter 2012, Washington D.C, USA Sabita Das

  13. Kinetic Freeze-out: Blast-Wave • Blast-Wave Model is used to fit the spectra • Two main parametersTkinand < β > • For central collisions: • Low temperature and high • flow velocity • For peripheral collisions: • High temperature and low • flow velocity STAR Preliminary STAR Preliminary STAR Preliminary STAR Preliminary Quark Matter 2012, Washington D.C, USA Sabita Das

  14. Kinetic Freeze-out: Tkin vs. <b> STAR Preliminary • Blast-Wave: Higher kinetic temperature corresponds to lower value of average • flow velocity and vice-versa. Quark Matter 2012, Washington D.C, USA Sabita Das

  15. Summary • New measurements for BES energies (39, 11.5 and • 7.7 GeV) at RHIC extend μB range from 20 - 400 MeV • of the QCD phase diagram • Chemical Freeze-out: Thermus model and particle ratios • First observation of centrality dependence of chemical • freeze-out parameters at lower energies • - Central collisions: GCE and SCE ~ Tch • - Peripheral collisions: Tch (SCE) > Tch (GCE) and • c2/ndf (SCE) > c2/ndf (GCE) at low energies • Kinetic Freeze-out: Blast-Wave model and Particle pT spectra • - Central collisions: Low Tkin and high <b> • - Peripheral collisions: High Tkin and low <b> STAR Preliminary Quark Matter 2012, Washington D.C, USA Sabita Das

  16. THANK YOU Quark Matter 2012, Washington D.C, USA Sabita Das

  17. Back up STAR Preliminary STAR Preliminary STAR Preliminary Quark Matter 2012, Washington D.C, USA Sabita Das

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