Centrality Dependence of Freeze-out Centrality Dependence of Freeze-out Parameters From the Beam Energy Scan at Parameters From the Beam Energy Scan at STAR STAR Sabita Das (for the STAR collaboration) Institute of Physics, Bhubaneswar, India Quark Matter 2012, Washington D.C, USA Sabita Das 06/23/22 1
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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 - PowerPoint PPT Presentation
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Centrality Dependence of Freeze-out Parameters From Centrality Dependence of Freeze-out Parameters From the Beam Energy Scan at STARthe Beam Energy Scan at STAR
Sabita Das (for the STAR collaboration)
Institute of Physics, Bhubaneswar, India
Quark Matter 2012, Washington D.C, USA Sabita Das04/20/23 1
OutlineOutline
Motivation
Introduction - Chemical freeze-out - Kinetic freeze-out
Experimental set-up
Particle Identification method
Results on freeze-out parameters
Summary
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das 2
STAR BES proposal: arXiv:1007.2613
- 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 , B and <> from identified particle spectra and ratios
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das 3
MotivationMotivation
QCD Phase Diagram
The main goals of RHIC BES program
IntroductionIntroduction
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das 4
Chemical Freeze-out : Inelastic collision ceases Particle ratios get fixed
★THERMUS : Statistical thermal model Ensemble used – Grand Canonical and Strangeness Canonical
€
ni =Tmi
2gi2π 2
(±1)k+1
kk=1
∞
∑ ekμ iT
⎛
⎝ ⎜
⎞
⎠ ⎟K2
kmiT
⎛
⎝ ⎜
⎞
⎠ ⎟
To consider incomplete strangeness equilibration:
Extracted thermodynamic quantities: ch, B, s and γS •Thermus, S. Wheaton & Cleymans, Comput. Phys. Commun. 180: 84-106, 2009.€
ni →niγ SSi
For Grand Canonical: Quantum numbers (B, S, Q) conserved on average
For Strangeness Canonical: Strangeness quantum number (S) conserved exactly
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das 5
Kinetic Freeze-out : Elastic collision ceases Transverse momentum spectra get fixed Blast Wave : Hydrodynamic inspired model
€
dN
pTdpT∝ rdrmT I0
pT sinhρ(r)
Tkin
⎛
⎝ ⎜
⎞
⎠ ⎟
0
R
∫ ×K1
mT coshρ(r)
Tkin
⎛
⎝ ⎜
⎞
⎠ ⎟
Extracted thermodynamic quantities: kin and <β>
E. Schnedermann et al., Phys. Rev. C 48, 2462 (1993)
IntroductionIntroduction
Particle spectra are fitted simultaneously
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das
The Solenoid Tracker At RHIC (STAR)The Solenoid Tracker At RHIC (STAR)
6
Data (2010): Au+Au 39GeV, 11.5 GeV and 7.7 GeV. Particles used : π p, Λ, Ξ and K0
S
TPCTPCTOFTOF
Full azimuthal particle identification.
Particle IdentificationParticle Identification
€
z = logdE /dx( )
meas.
dE /dx( )theory
⎛
⎝ ⎜ ⎜
⎞
⎠ ⎟ ⎟
€
m2 = p2 c2t 2
L2 −1 ⎛
⎝ ⎜
⎞
⎠ ⎟
p = momentum, t = time-of-flightc = velocity of light, L = path length
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das
TPC TPC+TOF
Coun
ts
Coun
tszπ m2 (GeV2/c4)
7
STAR Preliminary
STAR Preliminary
STAR Preliminary
STAR Preliminary
arXiv:1201.4203v1
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das 8
Particle SpectraParticle Spectra
arXiv:1201.4203v1 arXiv:1203.5183
STAR Preliminary STAR Preliminary
STAR PreliminarySTAR Preliminary STAR Preliminary
STAR Preliminary
Chemical Freeze-out Chemical Freeze-out
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das
Particles used : π, K, p, Λ Ξ and K0
s
Ensemble used: Grand Canonical
Fit parameters: ch s and γS
(strangeness saturation factor)
9
STAR Preliminary
STAR Preliminary
STAR Preliminary
STAR Preliminary
Particles used in the fit: π, K, p, Λ Ξ and K0s
Chemical freeze-out temperature increases with increase in collision energy. Baryon chemical potential decreases with increase in collision energy.
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das 10
Chemical Freeze-out Chemical Freeze-out
Au+Au 200 GeV : Phys. Rev. C 83 (2011) 24901
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das
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
11
Chemical Freeze-out Chemical Freeze-out
Au+Au 200 GeV : Phys. Rev. C 83 (2011) 24901
04/20/23 Quark Matter 2012, Washington D.C, USA Sabita Das 12
Chemical Freeze-out: Tch vs. B Chemical Freeze-out: Tch vs. B