Search for Preliminary Figures

Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb 70--80% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb 30--40% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb 0--5% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb 70--80% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb 30--40% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb 0--5% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from pp 70--80% multiplicity class collisions at $\sqrt{s} = 7\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from pp 30--40% multiplicity class collisions at $\sqrt{s} = 7\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from pp 0--5% multiplicity class collisions at $\sqrt{s} = 7\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from pp 70--80% multiplicity class collisions at $\sqrt{s} = 7\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from pp 30--40% multiplicity class collisions at $\sqrt{s} = 7\;\text{TeV}$
Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from pp 0--5% multiplicity class collisions at $\sqrt{s} = 7\;\text{TeV}$
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 0.9 TeV, 1D plots with fixed φₛₑₚ-s
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 13 TeV, 1D plots with fixed φₛₑₚ-s
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 7 TeV, 1D plots with fixed φₛₑₚ-s
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 5.02 TeV, 1D plots with fixed φₛₑₚ-s
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 2.76 TeV, 1D plots with fixed φₛₑₚ-s
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 13 TeV
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 7 TeV
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 5.02 TeV
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 2.76 TeV
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 0.9 TeV
Σ - 1 in pp collisions compared to phenomenological string model at √s = 0.9, 2.76 and 7 TeV
Σ - 1 in pp collisions compared to PYTHIA8 Monash2013 with ColourReconnection off at √s = 0.9, 2.76, 5.02, 7 and 13 TeV, and EPOS at √s = 13 TeV
Σ - 1 in pp collisions compared to PYTHIA8 Monash2013 tune at √s = 0.9, 2.76, 5.02, 7 and 13 TeV, and EPOS at √s = 13 TeV
Collision energy dependence of Σ - 1
Multiplicity class dependence of Σ - 1
The rapidity dependence of the second Fourier sine coefficient of the (Λ+Λ ̄) polarization along the beam direction in Pb-Pb collisions at √sNN = 5.02 TeV.
Transverse momentum dependence of the (Λ+Λ ̄) polarization along the beam direction in Pb-Pb collisions at √sNN = 5.02 TeV in semi-central collisions
Centrality dependence of the second Fourier sine coefficient of the (Λ+Λ ̄) polarization along the beam direction in Pb-Pb collisions at √sNN = 5.02 TeV
Fitting of second order sine Fourier coefficient of ⟨cos(θ*p⟩ as a function of invariant mass to estimate the (anti) lambda polarization along beam direction
Invariant mass distribution of anti-lambda candidates in Pb-Pb collisions at 5.02 TeV
The jet v2 as the function of trigger particle pT, compare to ATLAS jet trigger event v2 results
The positive significance of jet v2 as the function of trigger particle pT
The jet v2 as the function of trigger particle pT, compare to inclusive v2 in p-Pb collisions
The v2 distribution and fit of TPC-TPC pairs with 3< \it{p}_{\rm T}(trig)<5 GeV/\it{c}, 1.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
The v2 distribution and fit of TPC-TPC pairs with 2< \it{p}_{\rm T}(trig)<3 GeV/\it{c}, 1< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
The v2 distribution and fit of TPC-TPC pairs with 1.5< \it{p}_{\rm T}(trig)<2 GeV/\it{c}, 0.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
The jet signal fit and background fit in TPC-TPC correlation with 3< \it{p}_{\rm T}(trig)<5 GeV/\it{c}, 1.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
The jet signal fit and background fit in TPC-TPC correlation with 2< \it{p}_{\rm T}(trig)<3 GeV/\it{c}, 1< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
The jet signal fit and background fit in TPC-TPC correlation with 1.5< \it{p}_{\rm T}(trig)<2 GeV/\it{c}, 0.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
The TPC-TPC correlation and related fit in 3< \it{p}_{\rm T}(trig)<5 GeV/\it{c}, 1.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
The TPC-TPC correlation and related fit in 2< \it{p}_{\rm T}(trig)<3 GeV/\it{c}, 1< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
ZP vs. multiplicity in pp collisions at 13 TeV
ZN vs. multiplicity in pp collisions at 13 TeV
ZP vs. leading pT
ZN vs. leading pT
ZN spectrum in multiplicity bins in pp collisions at 13 TeV: ratio to MB
ZN spectrum in multiplicity bins in pp collisions at 13 TeV
p-side ZN signal vs. Ncoll in p-Pb collisions
p-side ZN signal vs. centrality in p-Pb collisions
Pb-side ZN signal vs. centrality in p-Pb collisions
ZDC asymmetry in multiplicity bins in pp collisions at 13 TeV
ZN and ZP asymmetry in pp collisions at 13 TeV
Very forward energy vs. multiplicity measured at midrapidity in pp and p-Pb collisions
ZDCA vs. ZDCC in pp collisions at 13 TeV
ZPA vs. ZPC in pp collisions at 13 TeV
ZNA vs. ZNC in pp collisions at 13 TeV
The TPC-TPC correlation and related fit in 1.5< \it{p}_{\rm T}(trig)<2 GeV/\it{c}, 0.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
Likelihood fit projections on invariant mass and pseudoproper decay length distributions (4 < pT < 5 GeV/c)
Fraction of J/ψ from beauty hadron decays in p-Pb collisions at 8.16 TeV in comparison with p-Pb measurements
Fraction of J/ψ from beauty hadron decays in p-Pb collisions at 8.16 TeV in comparison with pp measurements
Average-pT in NS-TS (Near Side/towards region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV.
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Average-pT in AS-TS (Away Side/region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV.
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle sum-pT density in AS-TS (Away Side/region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle sum-pT density in NS-TS (Near Side/towards region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle density in AS-TS (Away Side/region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle density in NS-TS (Near Side/towards region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle sum-pT density in Near Side (Toward region) for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle sum-pT density in Transverse Side/region for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle sum-pT density in Away Side/region for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle sum-pT density in Transverse Side/region for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle sum-pT density in Away Side/region for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb
Charged-particle sum-pT density in Near Side (Toward region) for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
  • PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
  • Energy: 5.02 TeV
  • System p-p ,
  • System p-Pb