long range rapidity correlations in high energy nucleus collisions at rhic and lhc
DESCRIPTION
Long range rapidity correlations in high energy nucleus collisions at RHIC and LHC. Heavy Ion Pub @ Ohsaka University Takahito Todoroki University of Tsukuba & Riken Nishina Center. Outline. Overview of basic ridge property Ridge study via Df correlations with respect to Reaction Plane - PowerPoint PPT PresentationTRANSCRIPT
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Long range rapidity correlations in high energy nucleus collisions at RHIC and LHC
Heavy Ion Pub @ Ohsaka University
Takahito Todoroki
University of Tsukuba & Riken Nishina Center
2011 Feb 18th 1T. Todoroki, University of Tsukuba
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Outline
• Overview of basic ridge property
• Ridge study via correlations with respect to Reaction Plane
• Triangular flow
• correlations with respect to trigger • Ridge in high multiplicity p+p events at LHC-CMS
• Summary
2011 Feb 18th T. Todoroki, University of Tsukuba 2
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Long range rapidity correlations
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Phys. Rev. C 80, 064912 (2009)
Jet Jet
Ridge
2< pTasso < pT
trig 2< pTasso < pT
trig
• Long range rapidity correlations up to large rapidity = “Ridge”
• Seen in Au+Au, absent in d+Au collisions
• Superposition of jet and ridge at in Au+Au collisions
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pT spectra of Jet and Ridge yield
• Jet spectrum is increasing with pTtrig as
jet fragmentation
• Ridge spectrum is softer and approximately independent of pT
trig
• Ridge is “bulk-like”
2011 Feb 18th T. Todoroki, University of Tsukuba 4
Phys. Rev. C 80, 064912 (2009)
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Ridge shape gets clearer with pT
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Centrality evolution of Ridge
• Rapid transition from 55-65% to 46-55%
• Small change to most central after transition
• Ridge may be phenomena of underlying event
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Au+Au 200GeV data - fit (except same-side peak)
46-55%
STAR Preliminary0-5%
STAR Preliminary
ηΔ width
M.Daughersity, QM08, J.Phys.G35:104090,2008pT > 0.15 GeV83-94% 55-65%
STAR Preliminary
STAR Preliminary
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Ridge and Jet correlations with respect to Reaction Plane
• Jet = () -Accep*()
• = near-side ridge + away-side
• Flow subtraction by ZYAM
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Ridge correlations have reaction plane dependence
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Correlated Emission Model
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in-planejet flow alignedmore ridge
out-of-planejet flow misalignedless ridge
Chiu,Hwa, arXiv:0809.3018Correlated Emission Model (CEM)
Asymmetric ridge peak predicted
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Ridge and Jet correlations with respect to Reaction Plane
• Jet = () -Accep*()
• = near-side ridge + away-side
• Flow subtraction by ZYAM
• 2 Gaussian fit to away side and subtracted
– Ridge obtained
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Near side peak asymmetry
• Jet shape is symmetric
• Ridge is asymmetric!
– shift to side
• Ridge may come from jet-flow alignment
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2
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Back to Back Ridge
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• Jet = () -Accep*()
• = near-side ridge + away-side
• Flow subtraction by ZYAM
• Fit : Back-to-Back Ridge + away conical emissions
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Triangular Flow
• Triangular flow is possible source of ridge!
2011 Feb 18th T. Todoroki, University of Tsukuba 13
arXiv:0806.0513v1
Pictures : Alver RHIC-AGS Meeting 2010
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Comparison of AMPT and STAR
• v2 & v3 are depending on initial geometry in AMPT
• AMPT simulations have good consistency with data at pT >0.8GeV
2011 Feb 18th T. Todoroki, University of Tsukuba 14arXiv:1003.0194v3
Vn= <cos n(assotrig)>~ Vn2
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S. Esumi WWND2011
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correlations with respect to trigger
• Jet and Ridge property as function of trigger – Back/Forward asymmetry of correlation shapes
– Gradient of correlation functions
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PYTHIA8
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AMPT
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0 ~
20%
20 ~
50%
50 ~
93%
trig= -2.0 trig= 2.0
C2 :
arbi
trar
y un
it
trig= 0
Near side :
assotrig:[-4,+4]
Flow Not Subtracted
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PHENIX Data Analysis
• Trigger “sign” selection : “” and “”
• Precise trigger selection : [-0.35,0.35] 14bins. 0.05 step.
• correlations : projected from correlations
– Near side : – Away side :
• Superposition of jet and ridge due to central arm accep.
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Trigger sign selected correlations
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Projected correlations : Trigger sign selected
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Near :
Away:
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Near side correlations : precise trigger selection
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Near :
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Away side correlations : precise trigger selection
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Away:
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Backward / Forward asymmetry
• Yield Ratio = (AvgForward - AvgBackward)/(AvgForward + AvgBackward)
– Forward : 0 < <0.25
– Backward : -0.25 < <0
• YR=0 : symmetric shape
• YR>0 or <0 : shift for Forward or Backward direction
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Backward Forward
“Forward” : >0“Backward” : <0
Centrality : 0~20trigger (hadron): Pt 2~4GeV trigassociate (hadron) : Pt 1~2GeV
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Backward / Forward asymmetry : trigger sign selection
• Degree of asymmetry
– at most 2in peripheral at near side
– at most 1in peripheral at away side
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Backward / Forward asymmetry : trigger precise selection
• Large statistical & systematic error on both near and away side
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Gradient of correlations as function of trig
• Fitting function : [0] + [1]*x
• Fitting range
– : [ 0,0.35] if trig <0
– : [-0.35,0] if trig <0
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if trig >0 if trig <0
Centrality : 0~20trigger (hadron): Pt 2~4GeV trigassociate (hadron) : Pt 1~2GeV
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Gradient of correlations seems to be flat
• Gradient of correlations seems to be flat at near side
• Away side also seems to be flat though still large statistical error
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Correlations in high multiplicity p+p events at LHC-CMS
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Back-to-back jet correlations enhanced in high multiplicity sample.
Minimum Bias no cut on multiplicity
High multiplicity data set and N > 110
The peak is truncated in both distributions
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Minimum Bias no cut on multiplicity
High multiplicity data set and N>110
New “ridge-like” structure extending to large at ~ 0
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Data and PYTHIA8
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Other simulation models
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Data and PYTHIAD6T at 0.9, 2.36 and 7 TeV
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PYTHIA D6T PT inclusive
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Comparison 7 TeV p+p and 200 GeV Cu+Cu correlations
• Correlations in Cu+Cu at similar multiplicity dominated by flow.
• How correlation shape changed if v2 exists in high mult. p+p event?
• Need to survey azimuthal dynamics in high mult. p+p events
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High multiplicity data set N>110Hard Probe 2010, Putschke
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Accumulative azimuthal correlations
• Consistent with p+p minimum bias at peripheral
• Enhance of Au+Au correlations at mid central & central by flow-like component
• Method to search the possible modification in high multiplicity p+p events from minimum bias because no event plane needed
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0.15 < pTasso <2.0GeV/c at
<i cos2(trig - iasso)> = Mult.*v2 (pT
trig) v2asso+{non-flow}
Trigger
arxiv:nucl-ex/0407007v3STAR AuAu 200GeV
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Midori Kajigaya Univ. of Tsukuba
Accumulative correlations in high multiplicity p+p events at 200 GeV
• Enhance in mid-rapidity high multiplicity event
• Azimuthal dynamics in p+p events depends on multiplicity if track number count and calculation done in same rapidity range.
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<i cos2(Pt - i)> = Mult.*v2 (pT) v2asso + {non-flow}
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Possible ridge in p+p collisions at RHIC energy?
• data to analyze : 500GeV, 200GeV and 62.4 GeV
2011 Feb 18th T. Todoroki, University of Tsukuba 37
CERN-ISR Nucl. Phys. B145 (1978) 305-348
p+p √s = 52.6 GeV0.5< Passo
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Summary
• Overview of basic ridge property
• Ridge study via correlations with respect to Reaction Plane
– Ridge depends on Reaction Plane
• Triangular flow
– Possible source of ridge
– AMPT well describes STAR experimental data at pT >0.8GeV
• correlations with respect to trigger – No trigger dependence seen in PHENIX acceptance…
• Ridge in high multiplicity p+p events at LHC-CMS
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Back Up Slides
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None trigger selected correlations
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