Measurements of Non-photonic Electrons at STAR · HF workshop, Utrecht (2012) - Mustafa Mustafa...
Transcript of Measurements of Non-photonic Electrons at STAR · HF workshop, Utrecht (2012) - Mustafa Mustafa...
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Measurements of Non-photonic Electrons
Production and Azimuthal Anistropy in STAR
at RHIC
Mustafa Mustafa
for the STAR Collaboration
Purdue University
5th International workshop on heavy quark production in
heavy-ion collisions, Utrecht
Results:
o NPE spectra measurements:
o New Au + Au at √sNN = 200 GeV.
o Nuclear Modification Factor at √sNN = 200 GeV.
o Au + Au at √sNN = 62.4 GeV.
o NPE Azimuthal Anisotropy measurements:
o v2 Au + Au at √sNN = 200 GeV.
o v2{2} Au + Au at √sNN =39 GeV and 62.4GeV.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 2
Why Heavy Flavor?
o Due to their large masses, heavy quarks are created at the
early stage of HIC through initial hard scattering
Leading order diagrams of charm (HQ) production.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 3
Why Heavy Flavor?
o Due to their large masses, heavy quarks are created at the
early stage of HIC through initial hard scattering, thus:
• pQCD cross-sections, power-law at high pT.
STAR Phys. Rev. D 86 (2012) 72013
Example: Charm production compared to FONLL calculation.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 4
Why Heavy Flavor?
o Due to their large masses, heavy quarks are created at the
early stage of HIC through initial hard scattering, thus:
• pQCD cross-sections, power-law at high pT.
• cross-sections scale by Nbin.
STAR Phys. Rev. D 86 (2012) 72013
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 5
Why Heavy Flavor?
o Due to their large masses, heavy quarks are created at the
early stage of HIC through initial hard scattering, thus:
• pQCD cross-sections, power-law at high pT.
• cross-sections scale by Nbin.
• experience all stages of medium evolution.
STAR Phys. Rev. D 86 (2012) 72013
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 6
Why Heavy Flavor?
o Due to their large masses, heavy quarks are created at the
early stage of HIC through initial hard scattering, thus:
• pQCD cross-sections, power-law at high pT.
• cross-sections scale by Nbin.
• experience all stages of medium evolution.
o Their masses are external to QCD.
STAR Phys. Rev. D 86 (2012) 72013
B. M
üll
er, N
ucl
. P
hys.
A, 750
(200
5),
p.
84–
97
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 7
Why Heavy Flavor?
o Due to their large masses, heavy quarks are created at the
early stage of HIC through initial hard scattering, thus:
• pQCD cross-sections, power-law at high pT.
• cross-sections scale by Nbin.
• experience all stages of medium evolution.
o Their masses are external to QCD.
STAR Phys. Rev. D 86 (2012) 72013
B. M
üll
er, N
ucl
. P
hys.
A, 750
(200
5),
p.
84–
97
Heavy Quarks are clean probes
(“almost” external to the “thermal” bulk matter)
to study the bulk matter created in heavy-ion collisions.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 8
Heavy Quarks as probes of sQGP
Heavy Quarks experience all the stages of medium evolution
their kinematics carry information about their interaction with the medium.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 9
Heavy Quarks as probes of sQGP
Heavy Quarks experience all the stages of medium evolution
their kinematics carry information about their interaction with the medium.
Observables:
o Modification of the power-law pT spectra (high pT)
• Study flavour dependence of partons energy loss.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 10
Heavy Quarks as probes of sQGP
Heavy Quarks experience all the stages of medium evolution
their kinematics carry information about their interaction with the medium.
Observables:
o Modification of the power-law pT spectra (high pT)
• Study flavour dependence of partons energy loss.
o Azimuthal Anistropy
• Low pT v2
degree of thermalization of the bulk matter.
NCQ-scaling? Hadronization mechanisms.
Important to understand Quarkonia production mechanisms in HIC.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 11
Heavy Quarks as probes of sQGP
Heavy Quarks experience all the stages of medium evolution
their kinematics carry information about their interaction with the medium.
Observables:
o Modification of the power-law pT spectra (high pT)
• Study flavour dependence of partons energy loss.
o Azimuthal Anistropy
• Low pT v2
degree of thermalization of the bulk matter.
NCQ-scaling? Hadronization mechanisms.
Important to understand Quarkonia production mechanisms in HIC.
• High pT v2
path length dependence of energy loss
(an important differential measurement to test parton energy loss models).
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 12
o Direct reconstruction through hadronic decay channels Allows direct access to the heavy quark kinematics.
• Hard to trigger.
• Limit the pT reach .
• Small(er) Branching Ratio: • 𝐵+ → 𝐾+ + 𝐽 𝜓 → 𝑒𝑒 : 𝐵𝑅: ~6 × 10−5
• 𝐵0 → 𝐾𝜋: 𝐵𝑅: ~5 × 10−6
• 𝐷0 → 𝐾𝜋: 𝐵𝑅:~4%
• 𝐷+ → 𝐾𝜋𝜋: 𝐵𝑅:~9.4% (lower acceptance)
0D
D0
K+
+
l
K-
e-/-
Reconstructing Open Heavy Flavour
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 13
Reconstructing Open Heavy Flavour
o Direct reconstruction through hadronic decay channels Allows direct access to the heavy quark kinematics.
• Hard to trigger.
• Limit the pT reach .
• Small(er) Branching Ratio: • 𝐵+ → 𝐾+ + 𝐽 𝜓 → 𝑒𝑒 : 𝐵𝑅: ~6 × 10−5
• 𝐵0 → 𝐾𝜋: 𝐵𝑅: ~5 × 10−6
• 𝐷0 → 𝐾𝜋: 𝐵𝑅:~4%
• 𝐷+ → 𝐾𝜋𝜋: 𝐵𝑅:~9.4% (lower acceptance)
o Indirect measurement through semi-leptonic decay channels • Indirect access to the heavy quark kinematics
Can be triggered easily.
• Ideal for high pT measurements
High(er) branching ratio
• 𝐵 → 𝑒+ +𝑋: 𝐵𝑅: ~10%
• 𝐷0 → 𝑒+ + 𝑋: 𝐵𝑅:~6.5%
• 𝐷+ → 𝑒+ +𝑋: 𝐵𝑅:~16%
• Λc → 𝑒+ + 𝑋: 𝐵𝑅: ~4.5% (Lightest charmed baryon)
0D
D0
K+
+
l
K-
e-/-
Non- photonic electron
0D
D0
K+
+
l
K-
e-/-
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 14
Experimental Setup
TOF BEMC Magnet
TPC
upVPD
BBC EEMC
The Solenoid Tracker At RHIC (STAR)
• Full azimuthal coverage.
• -1 < η < 1 • Uniform acceptance for all
beam energies.
• Full TOF barrel.
• Full BEMC
• Low material budget in the
tracking volume
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 15
Electrons Identification TPC dEdx +
Time Of Flight (TOF):
Low pT ( 0.2-2.0 GeV/c)
The combination of TPC dEdx and β
from TOF provides +95% purity down to
the lowest reachable pT at STAR
(0.2GeV/c) .
0
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 16
Electrons Identification TPC dEdx +
Barrel ElectorMagnetic Calorimeter
(BEMC):
High pT ( > 1 GeV/c)
1- Associating TPC tracks with BTOW
and BSMD clusters.
2- E/P cuts. (Due to their negligible
mass, electrons have E/P ~ 1).
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 17
Analysis Technique – Background Sources
The trick is to find all electrons and then subtract all the uninteresting ones.
Most of the “uninteresting” electrons are coming from photonic sources (Photonic Electrons).
ee
ee
0
BR: 1.2%.
BR: 0.7%.
ee
•Mostly from )(0
Same for all experiments
Depends on material budget
Other sources of background include:
• Drell-Yan and heavy quarkonia contributions (J/psi).
• Vector mesons di-electron decays (ρ,ω,Φ,…) .
• Single electron background sources, Ke3 (K+ → π0e+νe).
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 18
Analysis Technique – Background Subtraction
At STAR, we use the “Reconstruction Method”
to estimate the contribution of Photonic
electrons.
• Photonic e+e- pairs invariant mass peaks at 0.
• Almost all reconstructable pairs have
invariant mass < 0.24 GeV/c2 .
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 19
Analysis Technique – Background Subtraction
At STAR, we use the “Reconstruction Method”
to estimate the contribution of Photonic
electrons.
• Photonic e+e- pairs invariant mass peaks at 0.
• Almost all reconstructable pairs have
invariant mass < 0.24 GeV/c2 .
reco
purity
photonicNinclusiveNnpeN
)()(*)(
εpurity : purity of inclusive electrons
sample. Calculated from data.
εreco : photonic electrons reconstruction
efficiency. Calculated from embedding.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 20
Measurements in p + p at √sNN = 200 GeV
o p + p baseline.
STAR Phys. Rev. D 83 (2011) 052006
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 21
Measurements in p + p at √sNN = 200 GeV
o p + p baseline.
o NPE-hadron correlation.
used to disentangle charm and bottom
contribution to NPE spectra.
STAR Phys. Rev. D 83 (2011) 052006
ST
AR
PR
L 1
05
(2
01
0) 2
02
30
1
ST
AR
Ph
ys.
Rev
. D 8
3 (2
011
) 0
52
00
6
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 22
Spectra in Au + Au at √sNN = 200 GeV
o With ~1 nb-1 sampled luminosity in
Run2010 Au+Au collisions, STAR
provides a new measurement of
NPE with a highly improved result
at high pT.
o < (5-10)% statistical errors in all 4
centralities.
o An independent central trigger
provides 0-5% centrality.
p+
p N
PE
ST
AR
Ph
ys.
Rev
. D
83
(2
01
1)
05
20
06
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 23
Spectra in Au + Au at √sNN = 200 GeV
p+
p N
PE
ST
AR
Ph
ys.
Rev
. D
83
(2
01
1)
05
20
06
o With ~1 nb-1 sampled luminosity in
Run2010 Au+Au collisions, STAR
provides a new measurement of
NPE with a highly improved result
at high pT.
o < (5-10)% statistical errors in all 4
centralities.
o An independent central trigger
provides 0-5% centrality.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 24
Nuclear Modification Factor (RAA) in Au + Au at √sNN = 200 GeV
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 25
Nuclear Modification Factor (RAA) in Au + Au at √sNN = 200 GeV
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 26
Nuclear Modification Factor (RAA) in Au + Au at √sNN = 200 GeV
• Strong suppression at
high pT .
• Suppression increases
as a function of pT .
• RAA uncertainty is
dominated by
Run2005+Run2008
p+p uncertainty.
• Should be improved
with Run2009+2012
large statistics high
quality p+p data.
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0-10%
HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 27
Nuclear Modification Factor (RAA) in Au + Au at √sNN = 200 GeV
o Measurement at high pT clearly
disfavors radiative energy loss as the only mechanism.
DGLV: Djordjevic, PLB632, 81 (2006) and references within.
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0-10%
HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 28
Nuclear Modification Factor (RAA) in Au + Au at √sNN = 200 GeV
o Measurement at high pT clearly
disfavors radiative energy loss as the only mechanism.
o CUJET is the new improvement
over the DGLV/DGLV+EL efforts.
It is consistent with our
measurement.
DGLV: Djordjevic, PLB632, 81 (2006) and references within. CUJET: Buzzatti, arXiv:1207.6020
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0-10%
HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 29
o Measurement at high pT clearly
disfavors radiative energy loss as the only mechanism.
o CUJET is the new improvement
over the DGLV/DGLV+EL efforts.
It is consistent with our
measurement.
o All plotted energy loss mechanisms
agree with our measurement:
• T-Matrix.
• Collisional Dissociation.
• Ads/CFT.
Nuclear Modification Factor (RAA) in Au + Au at √sNN = 200 GeV
DGLV: Djordjevic, PLB632, 81 (2006) and references within. CUJET: Buzzatti, arXiv:1207.6020 T-Matrix: Van Hees et al., PRL100,192301(2008).
Coll. Dissoc. R. Sharma et al., PRC 80, 054902(2009). Ads/CFT: W. Horowitz Ph.D thesis.
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0-10%
HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 30
Looking at the current status of the different experimental measurements and theoretical predictions, it is clear that more differential
measurements are needed to distinguish
the different proposed mechanisms: • Bottom/charm measurement
separation.
• Simultaneous prediction of RAA and v2.
• Measurements and predictions of
centrality and pT dependence.
• Collision energy dependence.
Finally, one also needs to study:
• CNM. PHENIX, arXiv:1208.1293
• Charmed baryon enhancement. P.Sorenson, et al. PRC74, (2006) 024902
Martínez-García, et al. J.Phys.G 35 (2008)
044023
• Charmed mesons ratios D0/D, D+-/D,
Ds/D compared to production in vacuum.
Nuclear Modification Factor (RAA) in Au + Au at √sNN = 200 GeV
DGLV: Djordjevic, PLB632, 81 (2006) and references within. CUJET: Buzzatti, arXiv:1207.6020 T-Matrix: Van Hees et al., PRL100,192301(2008).
Coll. Dissoc. R. Sharma et al., PRC 80, 054902(2009). Ads/CFT: W. Horowitz Ph.D thesis.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 31
NPE v2 in Au + Au at √sNN = 200 GeV
Features:
o Finite v2 at low pT.
o Increasing v2 at
high pT.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 32
NPE v2 in Au + Au at √sNN = 200 GeV
Features:
o v2{EP} and v2{2}
agree in their
common pT
region.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 33
NPE v2 in Au + Au at √sNN = 200 GeV
Features:
o v2{4} is less
sensitive to non-
flow, puts a lower
limit on v2.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 34
NPE v2 in Au + Au at √sNN = 200 GeV
Features:
o D0 v2
measurement also
agrees with a finite
v2 at low pT.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 35
NPE v2 in Au + Au at √sNN = 200 GeV
Using different analysis and
techniques we have demonstrated that the v2
features we see are robust:
o Finite v2 at low pT is an
indication of strong charm-
medium interaction.
o Increase of v2 at high pT
possibly due to jet
correlation and pathlength
dependence of energy loss.
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o With the contribution of non-flow (jet correlations) at high pT it is difficult to
directly compare to models.
o It is interesting that the BAMPS model can reproduce the bump-feature we see at pT
1-2 GeV/c. Nevertheless, more precision is needed for decisive comparison to
models.
HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 36
NPE v2 in Au + Au at √sNN = 200 GeV
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 37
Spectra in Au + Au at √sNN = 62.4 GeV
To provide more experimental
discrimination power for
theoretical models STAR is
extending its NPE program to
lower energies.
The quest is to see if the energy
loss of heavy quarks
is lessened or turned o
at lower energies.
o J/ψ not subtracted.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 38
Spectra in Au + Au at √sNN = 62.4 GeV
o Measurement is systematically
higher than FONLL upper
limit.
o ISR measurement is consistent
with FONLL upper limit. IL NUOVO CIMENTO (1981), 65A, N4, 421-456
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 39
NPE v2{2} in Au + Au at √sNN = 62.4 and 39 GeV
39 and 62 GeV: v2{2}
consistent with zero at low-pT hinting at milder charm-
medium interaction at lower
energies compared to 200GeV.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 40
Summary of New Results
o New measurement of NPE in Au+Au at √sNN = 200GeV:
o High precision at high pT .
o RAA indicates strong suppression of heavy quarks, and disfavors radiative energy loss as
the only energy loss mechanism for heavy quarks.
o NPE Azimuthal Anisotropy shows a finite v2 at low pT this is an important indication of
strong charm-medium interaction.
o Possibly due to jet correlations and likely path-length dependence of energy loss, we
see an increasing in v2 towards high pT.
o NPE at lower energies: o NPE spectra in Au+Au √sNN = 62.4 GeV is systematically higher than FONLL.
o Measurement of NPE V2{2} at √sNN = 62.4 and 39GeV is consistent with zero at low
pT which might indicate a difference in the degree of charmed-medium interaction
compared to 200GeV.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 41
Backup Slides
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 42
Spectra in Au + Au at √sNN = 62.4 GeV
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o Measurement is systematically higher than FONLL upper limit.
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 43
Spectra in Au + Au at √sNN = 62.4 GeV –
NPE/Photonic Ratio
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HF workshop, Utrecht (2012) - Mustafa Mustafa (STAR) 44
NPE p + p at √s = 200 GeV
STAR Phys. Rev. D 83 (2011) 052006