CMS-PAS-HIN-16-017 | ||
Charge asymmetry dependence of elliptic and triangular flow in pPb and PbPb collisions at √sNN= 5.02 TeV | ||
CMS Collaboration | ||
February 2017 | ||
Abstract: Charge dependent elliptic azimuthal anisotropy (v2) in pPb and both v2 and triangular azimuthal anisotropy (v3) in PbPb collisions are measured at √sNN= 5.02 TeV with the CMS detector at the LHC. The normalized difference of v2 between positively and negatively charged particles, (v−2−v+2)/(v−2+v+2), shows a linear dependence with respect to the event-charged asymmetry Ach, with comparable slopes observed for pPb and PbPb collisions at similar multiplicities. In PbPb collisions, the slopes are found to be the same for the v2 and v3 coefficients within uncertainties. These observations pose a challenge to the hypothesis that the charge asymmetry dependence of v2 arises from a chiral magnetic wave. However, the results are in qualitative agreement with expectations based on local charge conservation. | ||
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CDS record (PDF) ;
inSPIRE record ;
CADI line (restricted) ;
These preliminary results are superseded in this paper, PRC 100 (2019) 064908. The superseded preliminary plots can be found here. |
Figures | |
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Figure 1:
Elliptic flow v2 for positive- and negative-charged particles as a function of charge asymmetry (left) and the normalized v2 difference, (v−2−v+2)/(v−2+v+2), as a function of corrected event charge asymmetry (right) for multiplicity range 185 ≤Nofflinetrk< 220 in PbPb collisions at 5.02 TeV. Statistical uncertainties are indicated by the error bars. |
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Figure 1-a:
Elliptic flow v2 for positive- and negative-charged particles as a function of charge asymmetry (left) and the normalized v2 difference, (v−2−v+2)/(v−2+v+2), as a function of corrected event charge asymmetry (right) for multiplicity range 185 ≤Nofflinetrk< 220 in pPb collisions at 5.02 TeV. Statistical uncertainties are indicated by the error bars. |
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Figure 1-b:
Elliptic flow v2 for positive- and negative-charged particles as a function of charge asymmetry (left) and the normalized v2 difference, (v−2−v+2)/(v−2+v+2), as a function of corrected event charge asymmetry (right) for multiplicity range 185 ≤Nofflinetrk< 220 in PbPb collisions at 5.02 TeV. Statistical uncertainties are indicated by the error bars. |
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Figure 2:
The event-averaged pT value (<pT>) for positive- and negative-charged particles as a function of charge asymmetry (left) and the normalized <pT> difference, (<pT>−−<pT>+)/(<pT>−+<pT>+), as a function of corrected event charge asymmetry (right) for multiplicity range 185 ≤Nofflinetrk< 220 in pPb and PbPb collisions at 5.02 TeV. Statistical uncertainties are covered by the data points. |
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Figure 2-a:
The event-averaged pT value (<pT>) for positive- and negative-charged particles as a function of charge asymmetry (left) and the normalized <pT> difference, (<pT>−−<pT>+)/(<pT>−+<pT>+), as a function of corrected event charge asymmetry (right) for multiplicity range 185 ≤Nofflinetrk< 220 in pPb collisions at 5.02 TeV. Statistical uncertainties are covered by the data points. |
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Figure 2-b:
The event-averaged pT value (<pT>) for positive- and negative-charged particles as a function of charge asymmetry (left) and the normalized <pT> difference, (<pT>−−<pT>+)/(<pT>−+<pT>+), as a function of corrected event charge asymmetry (right) for multiplicity range 185 ≤Nofflinetrk< 220 in PbPb collisions at 5.02 TeV. Statistical uncertainties are covered by the data points. |
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Figure 3:
The linear slope for v2 (left) and <pT> (right) parameters rnorm2 and rnorm<pT> as a function of event multiplicity in pPb and PbPb collisions at √sNN= 5.02 TeV. Statistical and systematic uncertainties are indicated by the error bars and shaded regions, respectively. |
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Figure 3-a:
The linear slope for v2 parameter rnorm2 as a function of event multiplicity in pPb and PbPb collisions at √sNN= 5.02 TeV. Statistical and systematic uncertainties are indicated by the error bars and shaded regions, respectively. |
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Figure 3-b:
The linear slope for <pT> parameter rnorm<pT> as a function of event multiplicity in pPb and PbPb collisions at √sNN= 5.02 TeV. Statistical and systematic uncertainties are indicated by the error bars and shaded regions, respectively. |
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Figure 4:
The triangular flow v3 for positive- and negative-charged particles (left) and the normalized difference in vn, (v−n−v+n)/(v−n+v+n), for n= 2 and n= 3 (right) as a function of corrected event charge asymmetry for 30-40% centrality of PbPb collisions at √sNN= 5.02 TeV. Statistical uncertainties are covered by the data points. |
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Figure 5:
The linear slope (rnormn) parameter for elliptic (n= 2) and triangular (n= 3) flow as a function of centrality for PbPb collisions at √sNN= 5.02 TeV. Statistical and systematic uncertainties are indicated by the error bars and shaded regions, respectively. |
Summary |
The charged-dependent elliptic flow coefficients (v2) in pPb and both v2 and triangular flow coefficients (v3) in PbPb have been measured as a function of event-charged asymmetry at √sNN= 5.02 TeV. The normalized slope parameters of v2 in pPb and PbPb collisions are found to be similar at the same event-charged particle multiplicities. Moreover, the normalized slope parameters of the v2 and v3 coefficients show similar magnitudes in various centralities. These observations would not be expected if the charge dependence resulted from a Chiral Magnetic Wave mechanism. The data are qualitatively consistent with predictions from the local charge conservation mechanism. |
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Compact Muon Solenoid LHC, CERN |
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