star fixed-target results from = 4.5 gev au+au and · 2017-09-26 · star fixed-target results from...
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STAR Fixed-Target Results from 𝑺𝑵𝑵 = 4.5 GeV Au+Au and 𝑺𝑵𝑵 = 4.9 GeV Al+Au Collisions
Muhammad Usman AshrafFor the STAR Collaboration
Tsinghua University, Beijing, P. R. China
September 23 Muhammad Usman Ashraf 1
Outlineq Goals of the BES-I Programq Physics Motivation of FXT program.q Introduction to the Fixed-Target (FXT)
Programq Results from Au+Au FXT Collisions
at 𝑆$$ = 4.5 GeV q Results from Al+Au FXT Collisions
at 𝑆$$ = 4.9 GeVq Future upgrades and the FXT programq Summary
September 23 Muhammad Usman Ashraf 2
STAR: arXiv:1007.2613
Goals of the BES Program
September 23 Muhammad Usman Ashraf 3
qBES phase I at RHICØStudy the onset of de-
confinement and phase boundary
ØSearch for the QCD critical point
ØTurn-off of QGP signalsØSoftening of the equation of
stateØFind evidence of the
possible first-order phase transition
qSystematic study of Au+Au collisions at 7.7, 11.5, 14.5, 19.6, 27, 39 GeV(BES Phase-I)
Motivation for the Fixed-Target Program
September 23 Muhammad Usman Ashraf 4
q NA49 has reported that the onset of deconfinement may occur at 7 GeV, the low end of BES range.
q How to achieve low energy?
Ø By installing a target inside the beam pipe and using RHIC beam as a projectile.
Ø It can extend the µ& range from 400 MeV to about 720 MeV
Ø Provide control measurements for searches of the critical point and onset of deconfinement
Need to probe lower energies!
M. Stephanov. J. Physics G.: Nucl. Part. Phys. 38 (2011) 124147 Need
datahere!
STAR PRELIMINARY
FXT
κσ2
Preliminary HADES result, Quark Matter 20170-10%(QM 2017)
Systematic uncertainties included
à FXT measurements needed to determine shape of kσ2
observable at lower energies
5
Peak behavior predicted in critical region:
Control Measurements for CEP Signatures
September 23 Muhammad Usman Ashraf
àGold foil is 1mm thick with about a 4% interaction probability
à1.3M Au+Au events with top 30% centrality trigger
àtarget is outside of the STAR TPC at ~211 cm
Fixed-Target Geometry
September 23 Muhammad Usman Ashraf 6
Results from FXT Au+Au Collisions
at 𝑺𝑵𝑵 = 4.5 GeV
September 23 Muhammad Usman Ashraf 7
Centrality Determination for Au+Au Collisions at 𝑺𝑵𝑵 = 4.5 GeV
Top5%
q nGoodTracks are those tracks which pass through basic QA cuts.
q Pileup has been removed by multiplicity cut.
q 15%-30% centralities are biased toward the more central collisions. This biasing is minimal for more central events.
September 23 Muhammad Usman Ashraf 8
STAR preliminary
FXT PID & Acceptance
9
Ke+e-π
p
d
t
3HeK
π
PID with Time-of-Flight DetectorPID with TPC
|p|/q (GV/c) |p|/q (GV/c)
dE/d
x (k
eV/c
m) 1/β
p T(G
eV/c
)
y y
TPC TPC
π π
e- e+ K Kp
dt
(GeV/c)π pp T (GeV
/c)
q In STAR, the acceptance for particles and anti-particles is the same. This is not normally true for an experiment with a dipole magnet.
Particle Reconstruction in Au+Au at 𝑺𝑵𝑵 = 4.5 GeV 𝐾() Λ
𝛯+
STAR preliminary STAR preliminary
STAR preliminary
π ,K, p are identified by dE/dx in TPC. Secondary vertex reconstruction.
September 23 Muhammad Usman Ashraf 10
Cou
nts
E895 data
K0S →π+ + π- Λ→ p + π
Ξ→ Λ+ π → (p + π) + π
0-5% 0-5%
0-30% 0-7%FWHM = 5.13 MeV
𝐾() -> π+ + π - Λ -> p + π
𝛯+ -> Λ + π -> (p + π) + πE895: PhysRevLett.91. (2003) 202301
Open symbols are reflected
π-
E895: Phys. Rev. C 68 (2003) 054905
E802: Phys. Rev. C 57 (1998) R466
E877: Phys. Rev. C 62 (2000) 024901
qAmplitudes and widths of the rapidity densities are consistent with results from the AGS experiments
Gaussian Fit
Systematic uncertainties Shown for STAR and E895
September 23 Muhammad Usman Ashraf 11
0-8% Central
0-4% Central
0-5% Central
0-5% Central
Pion Spectra and dN/dy Distribution
mT-m0 and dN/dy spectra of 𝑲𝑺𝟎 and Λ in Au+Au at 𝑺𝑵𝑵 = 4.5 GeV
September 23 Muhammad Usman Ashraf 12
(GeV/c)S0K-mTm
0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dm2)dN Tmπ2
ev1/(
N
10−10
9−10
8−10
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6−10
5−10
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3−10
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1−10
1
10
210 -1.5 < y < -1.25
-1.25 < y < -1.0
-1.0 < y < -0.75
-0.75 < y < -0.5
-0.5 < y < -0.25
STAR preliminary
Top 5%𝑲𝑺𝟎
)2 (GeV/cΛ-mTm0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dm2)dN Tmπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
5−10
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3−10
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1−10
1
10
-1.5 < y < -1.25
-1.25 < y < -1.0
-1.0 < y < -0.75
-0.75 < y < -0.5
-0.5 < y < -0.25
spectra Au+Au 4.5 GeVΛ-mT mΛ
STAR preliminary
ΛTop 5%
cmsy - y2− 1.5− 1− 0.5− 0 0.5 1 1.5 2
dN/dy
02468
101214 FXT STAR @ 4.5 GeVS
0K E917 @ 4.30 GeV+K E917 @ 4.30 GeV-K
)/2 E917 @ 4.30 GeV-+K+(K
STAR preliminary
Top 5%
cmy - y2− 1.5− 1− 0.5− 0 0.5 1 1.5 2
)/dy
ΛdN
(
02468
10121416 FXT STAR @ 4.5 GeVΛ
E891 @ 4.9 GeVΛ E877 @ 4.9 GeVΛ
STAR preliminary
Gaussian Fitting
Open symbols are reflected
Statistical Error only
Open symbols are reflected
Statistical Error only
Amplitudes and widths of rapidity density, dN/dy, are in a good agreement with AGS experiments.
Particle Yield comparison in Au+Au at 𝑺𝑵𝑵 = 4.5 GeV with different experiments
q The excitation function of integrated yield, dN/dy, at mid-rapidity, scaled by the average number of participants.
q 𝐾() points are scaled by factor of 10.q STAR data are in a good agreement with various AGS and CERN experiments.
September 23 Muhammad Usman Ashraf 13
§ E895: Phys. Rev. C 68 (2003) 054905
§ E895: NPA 698 (2002) 495c § E802: NPA 610 (1996) 139c § E877: Phys. Rev. C 63 (2001)
014902§ E891: PLB 382 (1996) 35 E896:
Phys. Rev. Lett. 88, 062301§ NA44: Phys. Rev. C 66 (2002)
044907 § NA49: JPG 30 (2004) S701§ NA49: Phys. Rev. Lett. 93 (2004)
022302 § Phys. Rev. Lett. 93 (2004) 022302 § NA57: JPG:NPP32 (2006) 2065§ WA98: Phys. Rev. C 67 (2003)
014906
PRELIMINARY
p π-
π+
10-30%10-25%
10-30%
STAR PRELIMINARY
STAR PRELIMINARY
STAR PRELIMINARY
Open symbols are reflected
Open symbols are reflected
Open symbols are reflected
Statistical errors only
Statistical errors only
Statistical errors only
September 23 Muhammad Usman Ashraf 14
q Proton flow is “positive”.q Pion flow is “negative”.q π+ flow is twice that of π-
flow.*15-30% centrality bias is not corrected.
Directed flow of protons and pions in Au+Au Collisions at 𝒔𝑵𝑵 = 4.5 GeV
𝑲𝑺𝟎
STAR PRELIMINARY
Open symbols are reflected
10-25%
slope near mid-rapidity-0.022 +- 0.015 Λ
STAR PRELIMINARY
Open symbols are reflected
10-30%
slope near mid-rapidity0.094 +- 0.015
Statistical errors only
Statistical errors only
September 23 Muhammad Usman Ashraf 15
qdv1/dy|y=0 of 𝐾() (mesons) is negative.qdv1/dy|y=0 of Λ (baryons) is positive.q*15-30% centrality bias is not corrected.
Directed flow of 𝑲𝑺𝟎 and Λ in Au+AuCollisions at 𝒔𝑵𝑵 = 4.5 GeV
STAR BES10-40%
STAR FXT10-25%
STAR PRELIMINARY
Statistical errors only
September 23 Muhammad Usman Ashraf 16
E895: PRL 84 (2000) 5488STAR: PRL 112 (2014) 162301
q First π results shown for this 𝑠$$ = 4.5 GeV. qThe mesons continue the trend of negative flow seen at higher
energies.
*15-30% centrality bias is not corrected
Directed Flow Comparison Across Experiments and Energies
September 23 Muhammad Usman Ashraf 17
q First π results shown for this energy range. qThe mesons continue the trend of negative flow seen at higher
energies.qProtons and Lambdas are consistent with positive flow indicative of
compression.
Directed Flow Comparison Across Experiments and Energies
BES-IICollider
E895: Phys. Rev. Lett. 84 (2000) 5488STAR: Phys. Rev. Lett. 112 (2014) 162301
*15-30% centrality bias is not corrected
STAR FXT10-25%
FXTSTAR PRELIMINARY
Elliptic Flow of Pions and Protons
FXT BES-IICollider
STAR PRELIMINARY
STAR PRELIMINARY
STAR PRELIMINARYE895: Phys. Rev. Lett. 83 (1999) 1295
p
Statistical Errors Only
Statistical Errors Only
Statistical Errors Only
September 23 Muhammad Usman Ashraf 18
0-30%
0-30%
q First measurement of pion elliptic flow for this energy range.
q Proton v2 shows good agreement with E895.
q *15-30% centrality bias is not corrected.
STAR PRELIMINARY
CERES: JPG30 (2004) S1371ALICE: PRL 110 (2013) 152301
STAR: PRC92 (2015) 21901
FXT BES-II
Systematic and statistical errors shown
September 23 Muhammad Usman Ashraf 19
q FXT measurement continues the decreasing trend towards lower energies and is in a good agreement with UrQMD.
Dynamical Relative Charge Number Fluctuations
Pion HBT Results STAR PRELIMINARY
STAR PRELIMINARY
E895: Phys. Rev. Lett. 84 (2000) 2798E866: Phys. Rev. C 66 (2002) 054096
STAR BES: Phys. Rev. C 92 (2015) 14904E895: Phys. Rev. Lett. 84 (2000) 2798E866: Phys. Rev. C 66 (2002) 054096 ALICE: Phys. Lett. B 696 (2011) 328
0-10% Central
0-15% Central
STAR PRELIMINARY
0.1 GeV/c < pT < 0.3 GeV/c
0.15 GeV/c < pT < 0.8 GeV/c
GeV/c2
Statistical Errors Only
Statistical Errors Only
Statistical Errors Only
September 23 Muhammad Usman Ashraf 20
0-10% Central
q Consistent with results from AGS experiments.
q In the FXT regime, as the collision energy rises, compression reduces the source size and increases the baryon density.
q The BES collider regime shows increased longitudinal expansion.
q First pion dv1/dy results obtained for this energy range. They continue the trend of negative flow for mesons.
q First pion v2 results obtained for this energy.
q First 𝜈dyn result obtained for this energy range.
q Spectra and yields, HBT radii, proton dv1/dy, and proton v2 results are consistent with results from AGS experiments.
à STAR operates well in FXT mode!
September 23 Muhammad Usman Ashraf 21
Conclusions from First FXT Run at 𝒔𝑵𝑵 = 4.5 GeV
Results from FXT Al+Au Collisions
at 𝑺𝑵𝑵 = 4.9 GeV
September 23 Muhammad Usman Ashraf 22
Centrality Determination for Al+Auat 𝑺𝑵𝑵 = 4.9 GeV
Top5%
q 3.4 M Al+Au events collected with the top 30% centrality.
q It is not a beam pipe study.
q Pileup has been removed by multiplicity cut.
September 23 Muhammad Usman Ashraf 23
nGoodTracks
Pileup
STAR preliminary
Data
Multiplicity0 50 100 150 200 250
Events
1
10
210
310
410
510
To
p 5
%T
op
10
%T
op
15
%T
op
20
%T
op
25
%T
op
30
%
Pil
e U
p
= 4.9 GeVNNsSTAR Al+Au GlauberPile Up
Particle Reconstruction in Al+Au at 𝑺𝑵𝑵 = 4.9 GeV
Al+Au at 𝑺𝑵𝑵 = 4.9 GeV, 0-5%
à K0S→π+ + π-
àΛ → p + π-
q π ,K, p are identified with TPC dE/dxq Secondary vertex reconstruction
𝐾() ΛSTAR preliminary STAR preliminary
September 23 Muhammad Usman Ashraf 24
0-5%0-5%
mT-m0 and dN/dy spectra of 𝑲𝑺𝟎 and Λ in Al+Au at 𝑺𝑵𝑵 = 4.9 GeV
September 23 Muhammad Usman Ashraf 25
)2 (GeV/cΛ-mTm0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dm2)dN Tmπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
5−10
4−10
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2−10
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1
10
210
-1.5 < y < -1.25
-1.25 < y < -1.0
-1.0 < y < -0.75
-0.75 < y < -0.5
-0.5 < y < -0.25
STAR preliminary
Top 5%
(GeV/c)S0K-mTm
0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dm2)dN Tmπ2
ev1/(
N
12−10
11−10
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-1.5 < y < -1.25
-1.25 < y < -1.0
-1.0 < y < -0.75
-0.75 < y < -0.5
-0.5 < y < -0.25
STAR preliminary
Top 5%
Λ𝑲𝑺𝟎
cmsy - y1.5− 1− 0.5− 0 0.5 1
)/dy
S0dN
(K
012345678
STAR Al+Au @ 4.9 GeVS0K Si+Au @ 5.39 GeV+K Si+Au @ 5.39 GeV-K
)/2 Si+Au @ 5.39 GeV-+K+(K
Au+Au 4.5 GeV
STAR preliminarySTAR data Top 5%
AGS data Top 7%
cmy - y1− 0.5− 0 0.5 1 1.5
)/dy
ΛdN
(
00.5
11.5
22.5
33.5
44.5
5 FXT STAR Al+Au @ 4.9 GeVΛ
STAR preliminary
Uncertainties are Statistical only
Amplitudes and widths of rapidity density, dN/dy, are In a good agreement with AGS experiments.
Uncertainties are Statistical only
Comparison of mT-m0 spectra and dN/dy with Au+Au and Al+Au
Ø mT-m0 Spectra and dN/dy in Different rapidity bins for FXT Au+Au collisions at 𝑺𝑵𝑵 = 4.5 GeV and Al+Au collisions at 𝑺𝑵𝑵 = 4.9 GeV.
Ø Errors are statistical only.à Solid line fit to data and dashed
line is extrapolation with fitting function.
September 23 Muhammad Usman Ashraf 26
)2 (GeV/cS0K-mTm
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2
-2dy
(GeV
/c)T
/dm2)d
NTmπ2
ev1/(
N
10−10
9−10
8−10
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-1.5 < y < -1.25
-1.25 < y < -1.0
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-0.75 < y < -0.5
-0.5 < y < -0.25
STAR preliminary
Open marker for Au+Au Solid marker for Al+Au
Top 5%
)2 (GeV/cΛ-mTm0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2
-2dy
(GeV
/c)T
/dm2)d
NTmπ2
ev1/(
N
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-0.5 < y < -0.25
STAR preliminary
Open marker for Au+Au Solid marker for Al+Au
Top 5%Λ𝑲𝑺𝟎
cmy - y2.5− 2− 1.5− 1− 0.5− 0 0.5 1 1.5 2 2.5
)/dy
ΛdN
(
02468
10121416 FXT STAR Au+Au @ 4.5 GeVΛ
E891 Au+Au @ 4.9 GeVΛ E877 Au+Au @ 4.9 GeVΛ FXT STAR Al+Au @ 4.9 GeVΛ
STAR preliminary
https://arxiv.org/pdf/1609.05102.pdfStar Note 0644 : Technical Design Report for the iTPC Upgrade Star Note 0666 : An Event Plane Detector for STAR
inner TPC upgrade
Event Plane Detector
endcap TOF
iTPC Upgrade:ü Improved dE/dx resolutionü Better momentum resolutionü Extends η coverage from
1.0 to 1.5 ü pT >60 MeV/cü Ready in 2019
EndCap TOF Upgrade:ü Mid-rapidity coverage is criticalü Needed for PID at mid-rapidityü -1.6<η<-1.1ü Allows higher energy range of
FXT programü Ready in 2019
EPD Upgrade:ü Better triggerü Reduces backgroundü Improves event plane
resolutionü 2.1<|η|<5.1ü Ready in 2018
September 23 Muhammad Usman Ashraf 27
The STAR Upgrades and the FXT program
q Detector upgrades required to extend STAR FXT up to 7.7 GeV, an overlap energy with the collider mode.
FXT Energy Reach With Upgrades
π
p T(G
eV/c
)
p T(G
eV/c
)
ylabylab
p
September 23 Muhammad Usman Ashraf 28
CurrentAcceptance
CurrentAcceptance
Acceptancewithupgrades
Acceptancewithupgrades
September 23 Muhammad Usman Ashraf 29
Need datahere!
BES-IICollider
Preliminary HADES result, Quark Matter 20170-10%(QM 2017)
STAR PRELIMINARY
FXT
Systematic uncertainties included
q 100 M (~2 days) events of Au + Au collisions at 𝑠33 = 3.0 GeV .
q The Event Plane Detector will be ready and available for flow analyses.
q Can obtain a fluctuation measurement at energies below BES-I.
Outlook: FXT Program in Run 18
September 23 Muhammad Usman Ashraf 30
q iTPC and eTOF upgrades will be available. q Would need 100 million events at each energy, 2 days per energy
(3.5 GeV – 7.7 GeV).q Data rate is limited by DAQ.q Data at 7.7 GeV would provide an overlap energy with the
collider mode.
Outlook: FXT Program in Run 19
C. Blume, J. Phys. G31, S57 (2005).
q Clear signals for 𝐾(), Λ and Ξ+ are observed in Au+Au at 4.5 GeV FXT test run
q Clear signals for 𝐾() and Λare observed in Al+Au at 4.9 GeV FXT test run.
q Have not seen Λ6 and 𝛀, due to low statistics.
q After upgrade we need ~100M events for each energy and hoping to see the Λ6, 𝛀 and Ξ+ .
September 23 Muhammad Usman Ashraf 31
Strange Particles in FXT and BES-II
Summaryq First FXT run results demonstrate STAR has a capability
to run in the fixed-target as well as in the collider mode. q Higher statistics FXT run in 2018 will allow a kurtosis
measurements at 3 GeV.q Installation of EPD in 2018 will allow to improve flow
measurements.q The FXT program will extend the energy range of the
RHIC BES-II down to √sNN = 3.0 GeV (𝜇B=720 MeV).q With detector upgrades the FXT program can be
extended up to 7.7 GeV, where it overlaps with the collider mode.
q This will also allow more comprehensive and refined measurements.
September 23 Muhammad Usman Ashraf 32
Thank You!
September 23 Muhammad Usman Ashraf 33
September 23 Muhammad Usman Ashraf 34
Back Up
E895_PRL86(2001)2533
STAR PRELIMINARY
E895_PRL86(2001)2533
Slope near mid-rapidity0.09 +/- 0.015
0-18%
Au+Au 3.8 GeV
Au+Au3.8 GeV
E895 trend:/p flow ratio at 4.5 GeV è 0.2
STAR FXT:/p flow ratio at 4.5 GeV è 1.1
Differences:E895 -- <px>STAR-FXT – v1
E895 – 0-18%STAR-FXT 10-25%
p
Λ
KE beam (AGeV)35
Comparison to E895 Λ Flow
Au+Au 4.5 GeV 10-25%
September 23 Muhammad Usman Ashraf
Λ
Λ
pT spectra of 𝑲𝑺𝟎 in Au+Au at 𝑺𝑵𝑵 = 4.5 GeV
Ø 𝐾() Spectra in Different rapidity bins for FXT Au+Au at 𝑺𝑵𝑵 = 4.5 GeV.Ø Statistical errors only.Ø 15-30% trigger is biased towards the most central.à Spectra are extrapolated to high pT with Stefan-Boltzmann fitting function.
September 23 Muhammad Usman Ashraf 36
(GeV/c)TP0 0.5 1 1.5 2 2.5
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/c)T
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ev1/(
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STAR preliminary STAR preliminary
[-1.25,-1.00]
STAR preliminary STAR preliminary STAR preliminary
[-1.00,-0.75] [-0.75,-0.50] [-0.50,-0.25]
STAR preliminary
[-1.50,-1.25][-1.75,-1.50]
pT spectra of Λ in Au+Au at 𝑺𝑵𝑵 = 4.5 GeV
Ø Λ Spectra in Different rapidity bins for FXT Au+Au at 𝑺𝑵𝑵 = 4.5 GeV.Ø Statistical errors only.Ø 15-30% trigger is biased towards the most central.à Spectra are extrapolated to high pT with Stefan-Boltzmann fitting function.
September 23 Muhammad Usman Ashraf 37
(GeV/c)TP0 0.5 1 1.5 2 2.5
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/c)T
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ev1/(
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(GeV/c)TP0 0.5 1 1.5 2 2.5
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(GeV
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ev1/(
N
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10
210
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)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
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10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
7−10
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10
210
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)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
STAR preliminary STAR preliminary
[-1.25,-1.00]
STAR preliminary STAR preliminary STAR preliminary
[-1.00,-0.75] [-0.75,-0.50] [-0.50,-0.25]
STAR preliminary
[-1.50,-1.25][-1.75,-1.50]
(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
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10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
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/c)T
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10
210
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(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
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ev1/(
N
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10
210
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)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
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(GeV
/c)T
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ev1/(
N
10−10
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10
210
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)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
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10
210
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)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
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STAR preliminary STAR preliminary
STAR preliminary STAR preliminary STAR preliminary
STAR preliminary
[-1.25,-1.00]
[-1.00,-0.75] [-0.75,-0.50] [-0.50,-0.25]
[-1.50,-1.25][-1.75,-1.50]
pT spectra of 𝑲𝑺𝟎 in Al+Au at 𝑺𝑵𝑵 = 4.9 GeV
(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5 4
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
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10
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spectra, Al+Au 4.9 GeVS0K
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
STAR preliminary
[-1.75,-1.50]
Ø 𝐾() Spectra in Different rapidity bins for FXT Al+Au at 𝑺𝑵𝑵 = 4.9 GeV.Ø Statistical errors only.à Spectra are extrapolated to high pT with Stefan-Boltzmann fitting function.
September 23 Muhammad Usman Ashraf 38
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
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8−10
7−10
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10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
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(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
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8−10
7−10
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10
210
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)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
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8−10
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10
210
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)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
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4−10
3−10
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1
10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
5−10
4−10
3−10
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10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
5−10
4−10
3−10
2−10
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1
10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
[-1.25,-1.00]
[-1.00,-0.75] [-0.75,-0.50] [-0.50,-0.25]
[-1.50,-1.25][-1.75,-1.50]
STAR preliminary STAR preliminary
STAR preliminary STAR preliminary STAR preliminary
STAR preliminary
pT spectra of Λ in Al+Au at 𝑺𝑵𝑵 = 4.9 GeV
(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5 4
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
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4−10
3−10
2−10
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1
10
210
spectra, Al+Au 4.9 GeVS0K
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
STAR preliminary
[-1.75,-1.50]
Ø Λ Spectra in Different rapidity bins for FXT Al+Au at 𝑺𝑵𝑵 = 4.9 GeV.Ø Statistical errors only.à Spectra are extrapolated to high pT with Stefan-Boltzmann fitting function.
September 23 Muhammad Usman Ashraf 39
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
5−10
4−10
3−10
2−10
1−10
1
10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
5−10
4−10
3−10
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1−10
1
10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
5−10
4−10
3−10
2−10
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1
10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
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(GeV
/c)T
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ev1/(
N
10−10
9−10
8−10
7−10
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5−10
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10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
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(GeV
/c)T
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ev1/(
N
10−10
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10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5
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(GeV
/c)T
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ev1/(
N
10−10
9−10
8−10
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10
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[-1.25,-1.00]
[-1.00,-0.75] [-0.75,-0.50] [-0.50,-0.25]
[-1.50,-1.25][-1.75,-1.50]
STAR preliminary STAR preliminary
STAR preliminary STAR preliminary STAR preliminary
STAR preliminary (GeV/c)TP
0 0.5 1 1.5 2 2.5 3 3.5
-2dy
(GeV
/c)T
/dP2)d
NTPπ2
ev1/(
N
10−10
9−10
8−10
7−10
6−10
5−10
4−10
3−10
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1
10
210
0-5%)-15-10% (x10
)-210-15% (x10)-315-20% (x10)-420-25% (x10)-525-30% (x10
(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
-2dy
(GeV
/c)T
/dP2)dN TPπ2
ev1/(
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10−10
9−10
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10
210
0-5%)-15-10% (x10
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(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
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(GeV
/c)T
/dP2)dN TPπ2
ev1/(
N
10−10
9−10
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10
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(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
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(GeV
/c)T
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ev1/(
N
10−10
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10
210
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(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
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(GeV
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ev1/(
N
10−10
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10
210
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(GeV/c)TP0 0.5 1 1.5 2 2.5 3 3.5
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(GeV
/c)T
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ev1/(
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10−10
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STAR preliminary STAR preliminary
STAR preliminary STAR preliminary STAR preliminary
STAR preliminary
[-1.25,-1.00]
[-1.00,-0.75] [-0.75,-0.50] [-0.50,-0.25]
[-1.50,-1.25][-1.75,-1.50]
Net-Proton Directed Flow Slope at Mid-rapidity
September 23 Muhammad Usman Ashraf 40
q A minimum is observed in the mid-rapidity slope of net proton directed flow.
q The energy range of this minimum is 𝑺𝑵𝑵 = 10-20 GeV.
q According to prediction of hydrodynamic models, this minimum resembles the “softest point”.
September 23 Muhammad Usman Ashraf 41
Centrality # of Events <Npart> +/- stat +/-sys
0-5% ~267k 335.9 +/- 0.51 +/-0.97
5-10% ~287k 285.9 +/- 0.56 +/-0.88
10-15% ~259k 242.4 +/- 0.53 +/-0.37
15-20% ~204k 203.9 +/- 0.48 +/-0.85
20-25% ~126k 170.3 +/- 0.44 +/-0.46
25-30% ~69k 142.2 +/- 0.43 +/-0.50
Relation between centrality bins and <npart>
September 23 Muhammad Usman Ashraf 42
Centrality PileUp Efficiency
0-5% 6.014710% 96.871020%
5-10% 2.179419% 95.604648%
10-15% 1.815579% 98.653689%
15-20% 1.578787% 96.707016%
20-25% 1.367026% 92.393202%
25-30% 1.149513% 95.157688%
Trigger efficiencies and pileup for each centrality bin.