heavy flavor measurements at rhic and lhc
DESCRIPTION
W. Xie (PURDUE University, West Lafayette). Heavy Flavor Measurements at RHIC and LHC. Motivations Heavy Quarkonia Open Heavy Flavor future perspective. l. Motivations. Sensitive to initial gluon density and gluon distribution at RHIC. produced mostly from gluon fusion - PowerPoint PPT PresentationTRANSCRIPT
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Heavy Flavor Measurements at RHIC and LHC
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W. Xie(PURDUE University, West Lafayette)
MotivationsHeavy QuarkoniaOpen Heavy Flavor future perspective
08/21/20132nd Workshop on Jet Modification
in the RHIC and LHC Era
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Motivations
Sensitive to initial gluon density and gluon distribution at RHIC. produced mostly from gluon fusion
Involve different interaction mechanisms from light quarks with the medium gluon bremsstrahlung radiation collisional energy loss collision dissociation Ads/CFT
Heavy quarkonia production reveals critical features of the medium. suppression from color screening or gluon
scattering enhancement from coalescence
Cold Nuclear effect.• Gluon shadowing , Color glass condensate,
Initial state Energy loss, etc 2
0D
D0
K+
lK-
e-/-
e-/-
e+/+
Heavy quarkonia
Open heavy flavor
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HF Measurements* vs. Energy
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39 62.4 193 200 2760 5020 7000
p+p
p(d)+A
A+A
√𝑆𝑁𝑁 (𝐺𝑒𝑉 )Coll. Spec.
* note: at RHIC and LHC
• Reference data missing in some energies.• interpolation based on pQCD. • Rely on other experiments or model predictions.
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Quarkonia Suppression: “Smoking Gun” for QGP
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Color Screening
cc
cc
J/y
D+
d
• Low temperature
• Vacuum
• High temperature
• High density
(screening effect take place)
Sequential meltinga QGP thermometerH. Satz, NPA 783 (2007) 249c.
d
D-
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The life of Quarkonia in the Medium can be Complicated
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• Observed J/y is a mixture of direct production+feeddown (R. Vogt: Phys. Rep. 310,
197 (1999)). – All J/y ~ 0.6J/y(Direct) + ~0.3 cc + ~0.1y’
– B meson feed down. • Important to disentangle different component
• Suppression and enhancement in the “cold” nuclear medium– Nuclear Absorption, Gluon shadowing, initial state energy loss, Cronin
effect and gluon saturation (CGC)– Study p+A collisions
• Hot/dense medium effect – J/ , y dissociation, i.e. suppression– Recombination, i.e. enhancement– Study different species, e.g. J/psi, – Study at different energy, i.e. RHIC, LHC
D+
cc
c
J/y
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Color singlet model (NNLO*CS): P. Artoisenet et al., PRL. 101, 152001
(2008), and J.P. Lansberg private communication.
LO CS+ color octet (CO): Y.-Q. Ma, et al.,, Phys. Rev. D84, 51
114001 (2011), and private communication
Color Evaporation Model: M. Bedjidian et al., hep-ph/0311048;
R. Vogt private communication
Quarkonia Production in p+p Collisions
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STAR: Phys. Rev. C80, 041902(R) (2009)STAR: JPG 38, 124107 (2011)PHENIX: Phys. Rev. D 82, 012001 (2010)
• Production mechanisms (J/psi) still need to be clarified.
• What’s the impact on production in AA collisions?
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PLB712 (2012) 165
Quarkonia Production in p+p Collisions
Multi-parton- interactions? CGC describe the data well.
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Quarkonia Production in p+p Collisions
Fraction of non-prompt J/psi ~scale with collisions energy Described well by CEM. (R. Vogt 4th IWHF 2011)
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J/ψ Production in d+Au 200 GeV
Significant suppression in forward region
Largely explained by shadowing+abs.
Predict different trend in backward region (Au direction) Cronin?
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ψ’ Production in d+Au 200 GeV
very different from J/psi on centrality dependence.
What LHC see?
Psi’ size ~2x J/psi.
Psi’ binding E ~0.1 x J/psi.
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CGC disfavored by data sys. Error mostly from p+p reference which is
from interpolation Mostly bin-by-bin correlated. Hard to say which is better:
shadowing, Eloss, etc Upsilon also suppressed in forward region. Similar to RHIC results.
Quarkonia Production in p+Pb 5.02 TeV
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pp reference not needed for RFB.
Shadowing + Eloss seems to describe the data better.
Quarkonia Production in p+Pb 5.02 TeV
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J/ψ Production in Au+Au 200 GeV
More suppression in forward region Larger CNM effect Re-generation?
Less suppression for higher pT Longer formation time? Cronin effect?
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J/ψ spectra in 200GeV Au+Au
Much smaller radial flow?Regeneration at low pT?
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Significantly less suppression at low pT at LHC.
N(cc@LHC) ~10x N(cc@RHIC)
Re-generation at LHC?
J/ψ spectra in 2.76 TeV Pb+Pb
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J/ψ spectra in 2.76 TeV Pb+Pb
More suppression at high pT than at low pT Consistent with the re-generation picture.
High pT J/psi suppression LHC > RHIC
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Comparing with the Lower Energy Results
Similar level of suppression from 20 – 200 GeV at all centrality and at all pT
Sequential melting?
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2S is suppressed.
1S is consistent with excited state suppression (~50% feeddown)
Regeneration could be significant
Upsilon Production in A+A Collisions
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Look at All Quarkonia Together
Low pT J/psi results seems to indicate contributions from re-generation.
High pT J/psi/psi’ and upsilon results seems to indicate a sequential melting picture.
Does the J/psi melt?
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Important to Study Open Heavy Flavor Production
• A good reference to quarkonia production– Similar initial state effect.
• CGC, Shadowing, initial state energy loss, etc.
– Large cross section (compared to J/ψ). • Accurate reference measurements.
• One of the most important probes for sQGP– Interactions between heavy quark and medium are quite
different from the ones for light quarks• gluon radiation, collisional energy loss, collisional disassociation, etc
– allow further understanding of the medium properties. – A “Gold Mine” to be fully explored soon.
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The Pros and Cons of Different Methods Direct reconstruction
allow direct access to the heavy quark kinematics, hard to trigger.
Limit the pT reach of the measurements small(er) Branching Ratio:
(lower acceptance)
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Indirect measurement through decays Indirect access to the heavy quark
kinematics Mixture of B and D contribution. can be triggered easily.
Ideal for high pT measurements High(er) branching ratio
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FONLL provide a good platform to describe Open HF in pp Collisions at RHIC and LHC
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Large CNM Effect Observed at RHIC
Large enhancement in d+Au collision at mid and backward rapidity.
small suppression at low pT at forward rapidity.
PHENIX HF e
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RpPb(NPE) systematically above 1.0, consistent with PHENIX
while RpPb(D) ~1.0.
Coincidence due to systematics or Be?
Consistent with the shadowing and CGC.
CNM Effects Observed at LHC
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• large suppression of high pT NPE suppress.
• Similar suppression level at RHIC and LHC.
• CNM seems to be responsible for the
ramp at pT< 5 GeV at RHIC
• RAA from QGP medium seems to be the same for HF and light quark
Non-photonic Electron Production A+A Collisions
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Note: J/psi not subtracted. seems to indicate no suppression at 62.4 GeV.
Cold nuclear effect?
Non-photonic Electron Production at Low Energy
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D0 Production in Au+Au 200 GeV
Suppression at high pT in central and mid-central collisions
Seems to be the same as pion suppression pattern at pT > 3 GeV/c. As observed in NPE results.
Enhancement at intermediate pT.
Radial flow due to coalescence OR CNM effect as part of NPE enhancement?
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D Meson Production in p+Pb 2.76 TeV
Similar level of suppression as RHIC for 2 < pT <6 GeV/c Within errors, follow light hadron suppression pattern
as indicated at RHIC. need more precision.
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B suppression in Au+Au 200 GeV
Based on NPE RAA at pT > 5 GeV/c and B fraction measurement.
B significantly suppressed
Based on NPE and D0 measurements Indicate suppression of B
Large uncertainty.
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(J/psi)
B suppression in Pb+Pb 2.76 TeV
• From non-prompt J/psi measurements.
• Significant B suppression observed.
• Even at most peripheral bin• shadowing?
• Suppression seems larger at forward rapidity region.
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pT (B meson: GeV/c)
Red: pT(J/) > 6 GeV/cBlue: pT(
cou
nts
PYTHIA6 default setting
What are the corresponding pT (B meson)
B meson significantly suppressed at 5-20 GeV/c at RHIC and LHC.
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Charm Suppressed More than Bottom
Comparison in similar pT region of B and D mesons.
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Large Heavy Flavor Elliptic Flow Observed
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At RHIC, low pT J/psi is suppressed rel. to open charm
High pT J/psi seems to follow the same suppression pattern as open charm
High pT J/psi NOT suppressed relative to open charm ?
H. Satz, arXic:1303.3493v2
Is it a fair to compare the two in same pT region?
Look at Open and Hidden Charm Together
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Comparison with Models
Current data placed some constraints on models Need PRECISION
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MTD (MRPC)
The Next Step: PRECISION
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backup
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Psi(2s) more suppressed at pT>6.5 GeV/c in |y|<1.6
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