Soumya Mohapatra for the ATLAS Collaboration Stony Brook University
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Transcript of Soumya Mohapatra for the ATLAS Collaboration Stony Brook University
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Measurement of elliptic and higher order flow at Pb+Pb Collisions
with the ATLAS detector2.76NNs TeV
Soumya Mohapatrafor the ATLAS CollaborationStony Brook University
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• Initial spatial fluctuations of nucleons lead to higher moments of deformations in the fireball, each with its own orientation.
• The spatial anisotropy is transferred to momentum space by collective flow
• The harmonics vn carry information about the medium: initial geometry, h/s
• Understanding of higher order vn can shed light on the physics origin of “ridge” and “cone” seen in 2P correlations
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
Introduction and Motivation
Singles:
Pairs:
EP method
2PC method
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• Tracking coverage : |h|<2.5• FCal coverage : 3.3<|h|<4.8 (used to determine Event Planes)
ATLAS Detector
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
|η|<2.5
3.3<|η|<4.8
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4Event Plane Method
Bands indicate systematic errors
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5Centrality dependence of vn
•5% Centrality bins + 0-1% centrality bin
•v2 has a stronger centrality dependence.
•Other vn are flatter.
•In most central collisions, v3,v4 can be larger than v2 at high enough pT
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• Similar trend across all harmonics (increase till 3-4GeV then decrease)• In most central collisions(0-5%): v3, v4 can be larger than v2.
pT Dependence of vn
Soumya Mohapatra : Stony Brook University
v nv n
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• Observe scaling: vn1/n =kv2
1/2, where “k” is only weakly dependent on pT.• R.Lacey et al. (http://arxiv.org/abs/1105.3782)
vn scaling
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
(vn 1
/n /v
21/2 )
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8vn from RHIC to LHC
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
FromXiaoyang GongQuark Matter 2011 Talk
vn(Ψn) vn(Ψn)
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9h Dependence of vn
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
•weak dependence on h (~5% drop within acceptance)
• For Correlations:
relation is true only if the h dependence is weak
,, v v va b a bn n n n
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10Two Particle Dh-Df correlationsNear-side jet peak is always visible
Ridge seen in central and mid-central collisions, weak h dependence
Away side has double hump structure in most central events
Peripheral events have near side peak truncated
Ridge strength first increases then decreases with centrality
Peripheral events have jet related peaks only
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11Obtaining harmonics from correlations
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
a) The 2D correlation function in Dh,Df.
b) The corresponding 1D correlation function in Df for 2<|Dh|<5 ( the |Dh| cut removes near side jet)
c) The vn,n obtained using a Discrete Fourier Transformation(DFT)
d)Corresponding vn values
( ( , v = v ,a a an T n n T Tp p p
Bands indicate systematic errors
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12Dh dependence of vn
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
•Repeat procedure in narrow Dh slices to obtain vn vs Dh.
•vn values peak at low Dh, due to jet bias.
•Relatively flat afterwards, so we require a |Dh| >2 gap (to remove near-side jet).
Bands indicate systematic errors
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13Universality of vn
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
vn,n is expected to factorize into single vn for flow
Obtain vn using “fixed pT” correlations
cross-check via “mixed-pT” correlation
Indeed, vn,n factorizes! (above certain Dh)
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14Comparison between the two methods
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
Centrality Dependence
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15pT Dependence of v2
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
The 2PC vn for |Dh|<0.5 deviates from the EP results (for all pT)
Good agreement seen for |Dh|>2 at pT<4 GeV.
See deviations for pT>4 GeV even for |Dh|>2 due to increased away-side jet contribution (which swings along Dh.
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16pT Dependence of other vn
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
We see similar trend as v2
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17Recovering the correlations from EP vn
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
From 2PC method From EP method
Chose v1,1 and normalization to be same as original correlation function, but all other harmonics are from EP analysis.
Correlation function is well reproduced, ridge and cone are recovered!
Common physics origin for the near and away-side long range structures.
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• Measured v2-v6 by both correlation and event-plane analysis. – Significant and consistent v2-v6 were observed by the two methods. – Measured in phase space much larger than at RHIC.– Each vn can act as independent cross-check for h/s.
• Noted that v2 doesn’t change drastically from RHIC to LHC
• Observed that the vn follow a simple scaling relation: vn1/n v∝ 2
1/2.
• Concluded that the features in two particle correlations for |Dh|>2 at low and intermediate pT (pT<4.0GeV) can be accounted for by the collective flow of the medium. – Double hump and ridge arise due to interplay of even and odd
harmonics
Summary
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
• ATLAS vn analysis note : http://cdsweb.cern.ch/record/1352458• ATLAS HI public results page : • https://twiki.cern.ch/twiki/bin/view/AtlasPublic/HeavyIonsPublicResults
For more results see:
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BACKUP SLIDES
BACKUP SLIDES
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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• Left panel: : v1(pTa) vs Dh for four fixed-pT correlations.
– We see that v1 ,1(pTa ) can become negative showing eta dependence of v1
• Right panel: v1(pTb) vs for target pT in (1.4,1.6) GeV
– We see that v1(pTb) depends on pT
a showing the breakdown of the scaling relation
Breakdown of v1,1 scaling
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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21Universality of vn
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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• Similar magnitude and pT dependence in overlapping pT range
v2 Comparison to RHIC
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
|η|<1
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• Charged hadrons, pT=0.5-20 GeV, mid-rapidity, |η|<1
v2 out to 20GeV
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
central
peripheral
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• pT evolution of two-particle Df correlations for 0-10% centrality selection, with a large rapidity gap (|Dh|>2) to suppress the near-side jets and select only the long range components.
pT evolution of Df correlations
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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25vn,n and vn vs Dh for other centralities
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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26pT Dependence of v3 (2PC)
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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27pT Dependence of v4 (2PC)
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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28pT Dependence of v5 (2PC)
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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• The EP is determined with the Q-vector method using E T flow in FCal
• In mid-central collisions, the Q2 vector is distributed in a ring-like structure indicating the excellent ability of the FCal in determining the reaction plane
• In Central and mid-central collisions and for higher harmonics, the ring blurs out
Q vector example
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
,1, ,
,
1cos( ) ; sin( ); tan ( )y nx n i i y n i i n
i i x n
QQ E n Q E n
n Qf f -
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The correlations are constructed by dividing foreground pairs by mixed background pairs.
Mixed background pairs account for detector acceptance. Final correlation contains only physical effects.
The detector acceptance causes fluctuations ~ 0.001 in the foreground pairs, which mostly cancels out in the ratio.
Two Particle Correlations
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
Foreground Pairs( )( )Mixed Pairs( )
C fffD
D D
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31Recovering 0-1% correlation
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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32Recovering 0-5% correlation
Soumya Mohapatra : Stony Brook University : ATLAS Collaboration
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Soumya Mohapatra : Stony Brook University : ATLAS Collaboration