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Probing the medium with photons. Outline:. Introduction. Motivation. Experiment. Results. Conclusion. Saskia Mioduszewski Ahmed Hamed. LBNL 21-05-07. Probing the medium High-p T Spectra I – Light quarks and gluons. Mid-rapidity. Statistical Method. Photons. - PowerPoint PPT Presentation
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Probing the medium with photons
Outline:Outline:
oMotivation
oExperiment
oResults
oConclusion
oIntroduction
LBNL 21-05-07LBNL 21-05-07
Saskia MioduszewskiAhmed Hamed
2
Probing the medium High-pT Spectra I – Light quarks and gluons Probing the medium High-pT Spectra I – Light quarks and gluons
The suppression of 0,s and ,s is
very similar.suppression occurs at the parton level.
The binary scaling of
direct photons is strong
evidence that suppression is not
an initial state effect.
Mid-rapidity
Statistical Method
LBNL 21-05-07LBNL 21-05-07
<E> sCxqL^ 2 “Static medium”
yT es
px 2
~ Gluons dominance at mid-rapidity at RHIC energy.
PhotonsPHENIX, QM05
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QCD is flavor independent, but
heavy quarks at same pT are moving
much slower than light quarks.
Expected “dead-cone” with no induced
gluon radiation.
Non photonic electrons-Charm and Beauty
LBNL 21-05-07LBNL 21-05-07
Probing the medium High-pT Spectra II– Heavy quarks and gluons Probing the medium High-pT Spectra II– Heavy quarks and gluons
osingle-particle suppression does not constrain the mechanism of energy loss.
osingle-particle suppression in AuAu is strong evidence for the hot and
dense medium formation.
nucl-ex/0607012
4LBNL 21-05-07LBNL 21-05-07
Baryons and Mesons
Clear meson-baryon yield differences at intermediate pT .
Probing the medium High-pT Spectra III– quarks and gluons Probing the medium High-pT Spectra III– quarks and gluons
No reduction is observed in the baryon/meson ratio as expected in the gluon dominance picture.
Calibrated probe of the QGP is needed for better understanding of energy loss.
STAR QM05 and nucl-ex/0601042
5LBNL 21-05-07LBNL 21-05-07
?
Near-side: p+p, d+Au, Au+Au
is similar.Back-to-back: Au+Au
strongly suppressed relative to p+p and d+Au.Suppression of the
back-to-back correlation in central Au+Au is a final-state
effect
Probing the medium Jet-like azimuthal correlationsProbing the medium Jet-like azimuthal correlations
LBNL 21-05-07LBNL 21-05-07
Surface bias for the trigger particle.
Trigger particle with no surface bias is required for better quantitative measurements of the away-side modifications.
Charged hadrons
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Introduction SummaryIntroduction Summary
LBNL 21-05-07LBNL 21-05-07
Better understanding for the energy loss mechanism!
Elliptic flow.
oDirect Photons:
Gamma-charged hadrons correlation.
Four multipurpose experiments (BRAHMS, PHENIX, PHOBOS, STAR) Empirical lines of evidence:
Energy density well beyond critical value.Large elliptic flow. Jet quenching. dAu control experiment.
Interpreted in terms of a strongly coupled QGP and a new QCD state (?) Color Glass Condensate
Required:
Challengeable measurements!
Doesn’t couple to the medium.QGP thermal photons.
Test for binary scaling for hard process.
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Motivation LO Direct photonsMotivation LO Direct photons
Bremsstrahlung
fragmentation component
direct component
Decay photons
nT
1
phard:
/ E Tethermal:
schematic view
Calibrated probe of the QGP – at LO.
No Surface Bias Hard process
single-particle suppression does not effectively constrain detailed energy-loss pictures.
LBNL 21-05-07LBNL 21-05-07
Possible candidate for quark/gluon jet discrimination at LO.
oGamma-charged hadrons correlation.
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Experiment STAR DetectorExperiment STAR Detector
Tracker detectors(slow), Trigger detectors(fast), and Calorimeters(fast).
LBNL 21-05-07LBNL 21-05-07
Measurements of hadrons production over a large
solid angle.
STAR BEMC can probe for further higher transverse
energy.
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Experiment STAR BEMCExperiment STAR BEMCC
ross-s
ecti
on
in
LBNL 21-05-07LBNL 21-05-07
o120 modules.
o4800 channels
oSMDs: 36000 channels
oPreShower: 4800 channels
oLead-scintillator detector.
oSampling calorimeter.
oProjective towers.
Cro
ss-s
ecti
on
in
BEMC face is
~2.2m away
from the point of interaction
at =0.
West side 0<<1
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Experiment Electromagnetic ShowerExperiment Electromagnetic Shower
LBNL 21-05-07LBNL 21-05-07
-plan
e
-plane
E M C M o d u le
= 0
= 1+
S h o w e r M a xd e te c to r
To w e r
w ire s
w ire s
P re S h o w e r
A . A . P. S u a id e
High energy core.Low energy halo.
Electromagnetic transverse shower characteristics
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Inclusive-jet in Au+Au at s=200GeV
Thomas DietelQuark Matter
2005
Results QM 2005Results QM 2005
LBNL 21-05-07LBNL 21-05-07
SIMULATION (pp)
The background is higher for central events.Away-side decreases with increasing centrality.Decrease in near-side due to the increased
fraction of prompt photons.Need /0 discrimination.
STAR Preliminary
Simulation shows no associated particles in -charged correlation.
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Results QM 2006Results QM 2006
S. ChattopadhyayQuark Matter
2006
LBNL 21-05-07LBNL 21-05-07
Reduction in near angle peak towards photon Bin.Effect is more prominent for larger Et
trigger .Away-side yield is reduced.
pp at s=200GeV
STAR Preliminary
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Results Transverse Shower ProfileResults Transverse Shower Profile
LBNL 21-05-07LBNL 21-05-07
Clear structure for the two showers in and 0
at moderate energy.
0 shower at high energy is still wider
than the single photon shower.
Could be used to distinguish 0/
Clear sensitivity to the halo region.
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cucu 0-10%
Et_trg>12GeV
Et_trg>6GeV
/c
/c /c
(rad)
(rad)
(rad)
(rad)
/c0
Results Raw correlation functionResults Raw correlation function
LBNL 21-05-07LBNL 21-05-07
Preliminary
Similar Away-side for 0 and
Reduction in the near-side for compared to 0.
Reduction is more noticeable at higher Et_trg
and also at higher centrality bins.
d
1
Ntrg
dN()
Y-axis:
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Conclusion Conclusion
LBNL 21-05-07LBNL 21-05-07
-charged hadrons correlation is very promising tool for better understanding of the medium.
Shower shape study is required for direct photons identification.
Promising study for transverse shower profile is undertaken.
Comparison with the previous study of transverse shower profile is necessary.
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Thank you all
Thanks to Texas A&M nuclear physics group.
Thanks to all STAR Collaborators