| 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 $\sqrt{s} = 7\;\text{TeV}$
|
|
| 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
|
|
