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Public Preliminary figures by analysis

Characterizing system dynamics with two-particle transverse momentum correlations in pp, p--Pb, and Pb--Pb collisions

Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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 $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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 $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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 $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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 $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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 $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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 $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Charged particle multiplicity evolution of the azimuthal 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 $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
Charged particle multiplicity evolution of the azimuthal 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 $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
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 $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
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 $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
Charged particle multiplicity evolution of the azimuthal 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 azimuthal 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 $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
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 $\sqrt{s} = 7\;\text{TeV}$

Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ

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

Lambda baryon polarization along beam direction in Pb-Pb collisions at 5.02 TeV

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

v2 of jet particles in p-Pb and 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}

ZDC vs. midrapidity activity analysis

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