| Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 10< pT,jet<15 GeV/c in pp 13 TeV
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| Angular correlation functions for unlike-sign pairs of pions, kaons and protons
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| Angular correlations of like-sign particles (pions, kaons, protons) in pp collisions at 13 TeV
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| Projections of angular correlation functions for unlike-sign pairs of pions, kaons and protons
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| Projections of angular correlation functions for like-sign pairs of pions, kaons and protons
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| Eta - Ratio of individual measurements to combined - 0-10% centrality - PbPb 5TeV
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| Eta to pi0 ratio - in-jet and MB - pp 5TeV
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| Eta - in-jet and MB production - pp 5TeV
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| Pi0 - in-jet and MB production - pp 5TeV
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| $p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential proton-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential proton-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential phi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| $p_\textrm{T}$-differential phi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| Low-mass dielectron pT,ee (PYTHIA+EPS09, 1.04 < mee < 2.4, pt > 0.2)
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| $p_\textrm{T}$-differential phi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
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| Cross section of heavy-flvaour jets with electrons in pp at 5.02 TeV with POWHEG (R=0.6)
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Low pT,ee spectrum in 0-40% centrality with calculations for thermal and photo-production dielectrons.
- Fig. Group : low pTee spectra
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System Pb-Pb
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Low pT,ee spectrum in 70-90% centrality with calculations for thermal and photo-production dielectrons.
- Fig. Group : low pTee spectra
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System Pb-Pb
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| Toward pT spectra
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RpPb jpsi at mid-rapidity in comparison with preliminary result at 5 TeV (min bias data)
- Fig. Group : p-Pb 8 TeV min bias
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 8 TeV
- System p-Pb
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| Anti-deuteron inelastic interaction cross-section with ALICE material
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| Anti-proton inelastic interaction cross-section with ALICE material
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Low pT,ee spectrum in 0-40% centrality with Rapp prediction
- Fig. Group : low pTee spectra
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System Pb-Pb
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Low pT,ee spectrum in 70-90% centrality with Rapp prediction
- Fig. Group : low pTee spectra
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System Pb-Pb
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Comparison of J/ψ yield at mid and forward rapidity, as a function of the charged particle multiplicity densities at mid-rapidity
- Fig. Group : J/psi->mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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Low pT,ee spectrum in 0-40% centrality
- Fig. Group : low pTee spectra
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System Pb-Pb
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Low pT,ee spectrum in 70-90% centrality
- Fig. Group : low pTee spectra
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System Pb-Pb
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pt differential RpPb jpsi at mid-rapidity (min bias data) at 8TeV in comparison with theory calculations
- Fig. Group : p-Pb 8 TeV min bias
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 8 TeV
- System p-Pb
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pt differential RpPb jpsi at mid-rapidity (min bias data) at 8TeV
- Fig. Group : p-Pb 8 TeV min bias
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 8 TeV
- System p-Pb
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RpPb jpsi at mid-rapidity in comparison with muon result at 8 TeV (min bias data) and theory calculations
- Fig. Group : p-Pb 8 TeV min bias
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 8 TeV
- System p-Pb
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RpPb jpsi at mid-rapidity in comparison with muon result at 8 TeV (min bias data)
- Fig. Group : p-Pb 8 TeV min bias
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 8 TeV
- System p-Pb
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| RpPb for D0-tagged jets at 5.02 TeV, linear scale on x-axis (for comparison with RAA, part 1)
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| Xi to Lambda Ratio in jet within pp with jet R=0.4 Matching R=0.4
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| Scope: PAG Lambda to Kshort Ratio in jet within pp with jet R=0.4 Matching R=0.4
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Dielectron mass spectra in pp (7 and 13 TeV) and PbPb (2.76 and 5.02 TeV) collisions
- Fig. Group : Low Mass -> e+e-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 2.76 TeV
, - Energy: 5.02 TeV
, - Energy: 7 TeV
, - Energy: 13 TeV
- System p-p ,
- System Pb-Pb
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| RpPb and RAA for D0-tagged jets at 5.02 TeV, linear scale on x-axis
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Comparison of Υ(1S) and Y(2S) yields at forward rapidity, as a function of the charged particle multiplicity at mid-rapidity
- Fig. Group : Upsilon -> mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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Bottomonium production rate as a function of charged particle multiplicity
- Fig. Group : Upsilon -> mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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|
Υ(2S) yield at forward-rapidity as a function of the charged particle multiplicity at mid-rapidity with the deviation from linearity
- Fig. Group : Upsilon -> mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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|
Y(2S) yield at forward-rapidity as a function of the charged particle multiplicity densities at mid-rapidity
- Fig. Group : Upsilon -> mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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|
Comparison of Υ(1S) and J/ψ yields at forward rapidity, as a function of the charged particle multiplicity at mid-rapidity
- Fig. Group : Upsilon -> mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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|
Υ(1S) yield at forward-rapidity as a function of the charged particle multiplicity at mid-rapidity with the deviation from linearity
- Fig. Group : Upsilon -> mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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|
Υ(1S) yield at forward-rapidity as a function of the charged particle multiplicity densities at mid-rapidity
- Fig. Group : Upsilon -> mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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|
J/ψ yield at forward-rapidity as a function of the charged particle multiplicity densities at mid-rapidity with the deviation from linearity
- Fig. Group : J/psi->mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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| Reconstruction efficiency of D0-tagged charged jets, pp at 5.02 TeV (Run2)
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| Raw D0-tagged charged jets pT distributions, D0 pT intervals, pp at 5.02 TeV (Run2)
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| D0-tagged charged jets: invariant mass distributions in 3 D0 pT intervals, pp at 5.02 TeV (Run 2)
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| RpPb for D0-tagged jets at 5.02 TeV
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| Cross section of D0-tagged charged jets (anti-kT, R=0.3) with pT,D > 3 GeV/c, in pp and p-Pb at 5.02 TeV
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| RpPb and RAA for D0-tagged jets at 5.02 TeV
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| Cross section of D0-tagged jets in pp at 5.02 TeV
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| Dielectron spectrum with Rapp predictions
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| Dielectron spectrum with PHSD predictions
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|
J/ψ yield at forward-rapidity as a function of the charged particle multiplicity densities at mid-rapidity
- Fig. Group : J/psi->mu+mu-
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System p-p
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| Eta/Pi0 in pPb collisions at 5TeV with K/pi - 0-20 & 60-100% V0A
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| Eta/Pi0 in pPb collisions at 5TeV - ZNA sliced
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| Eta/Pi0 in pPb collisions at 5TeV - CL1 sliced
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| Eta/Pi0 in pPb collisions at 5TeV - V0A sliced
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| Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 60-100 % V0A
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| Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 60-100 % CL1
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| Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 60-100 % ZNA - Hybrid Ncoll
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| Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 0-20 % ZNA - Hybrid Ncoll
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| Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 0-20 % V0A
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| Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 0-20 % CL1
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| Eta Meson QpPb in pPb collisions at 5TeV - ZNA sliced - Hybrid Ncoll
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| Eta Meson QpPb in pPb collisions at 5TeV - V0A sliced
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| Eta Meson QpPb in pPb collisions at 5TeV - CL1 sliced
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| Neutral Pion QpPb in pPb collisions at 5TeV - ZNA sliced - Hybrid Ncoll
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| Neutral Pion QpPb in pPb collisions at 5TeV - CL1 sliced
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| Neutral Pion and Eta Meson Invariant Yield in pPb collisions at 5TeV compared to generators - 40-60% V0A
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| Neutral Pion and Eta Meson Invariant Yield in pPb collisions at 5TeV compared to generators - 20-40% V0A
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| Neutral Pion and Eta Meson Invariant Yield in pPb collisions at 5TeV compared to generators - 60-100% V0A
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| Neutral Pion and Eta Meson Invariant Yield in pPb collisions at 5TeV compared to generators - 0-20% V0A
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| Eta Meson Invariant Yield in pPb collisions at 5TeV - V0A sliced
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| Eta Meson Invariant Yield in pPb collisions at 5TeV - CL1 sliced
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| Eta Meson Invariant Yield in pPb collisions at 5TeV - ZNA sliced
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| Neutral Pion Invariant Yield in pPb collisions at 5TeV - ZNA sliced
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| Neutral Pion Invariant Yield in pPb collisions at 5TeV - CL1 sliced
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| Neutral Pion Invariant Yield in pPb collisions at 5TeV - V0A sliced
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| Dielectron spectrum with cocktail incl EPS09-modified charm
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| Dielectron spectrum with cocktail incl EPPS16-modified charm
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| Dielectron spectrum with cocktail incl binary scaled charm
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