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Public Preliminary figures by analysis

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ID number ALI-PREL-XXX

Figure Caption

Scope: PWG

System

Energy

Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)

Average values of mean pT in Backward window as a function of mean pT in Forward window: centrality class of 80% width (by V0M) in Pb-Pb collisions at 2.76 TeV

Fig. Group : Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)
PWG : PWG-CF (Flow and Correlations)
Energy: 2.76 TeV
System: Pb-Pb

Average values of mean pT in Backward window as a function of mean pT in Forward window: several centrality classes of 40% width (by V0M) in Pb-Pb collisions at 2.76 TeV

Fig. Group : Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)
PWG : PWG-CF (Flow and Correlations)
Energy: 2.76 TeV
System: Pb-Pb

Average values of mean pT in Backward window as a function of mean pT in Forward window: several centrality classes of 20% width (by V0M) in Pb-Pb collisions at 2.76 TeV

Fig. Group : Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)
PWG : PWG-CF (Flow and Correlations)
Energy: 2.76 TeV
System: Pb-Pb

Average values of mean pT in Backward window as a function of mean pT in Forward window: several centrality classes of 10% width (by V0M) in Pb-Pb collisions at 2.76 TeV

Fig. Group : Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)
PWG : PWG-CF (Flow and Correlations)
Energy: 2.76 TeV
System: Pb-Pb

Average values of mean pT in Backward window as a function of mean pT in Forward window: several centrality classes of 5% width (by V0M) in Pb-Pb collisions at 2.76 TeV

Fig. Group : Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)
PWG : PWG-CF (Flow and Correlations)
Energy: 2.76 TeV
System: Pb-Pb

Strength of event-mean transverse momenta correlations (bcorr) in centrality classes of 5% width in Pb-Pb collisions at 2.76 TeV at three η-gaps 0, 0.6 and 1.2 in comparison with AMPT

Fig. Group : Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)
PWG : PWG-CF (Flow and Correlations)
Energy: 2.76 TeV
System: Pb-Pb

Strength of event-mean transverse momenta correlations (bcorr) in centrality classes (2% width) by V0M, ZDCvsZEM and CL1 in Pb-Pb collisions at 2.76 TeV

Fig. Group : Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)
PWG : PWG-CF (Flow and Correlations)
Energy: 2.76 TeV
System: Pb-Pb

Strength of event-mean transverse momenta correlations (bcorr) in centrality classes (5% width) by V0M, ZDCvsZEM and CL1 in Pb-Pb collisions at 2.76 TeV

Fig. Group : Forward-backward correlations between event-mean transverse momenta in Pb-Pb collisions (QM2017 and IS2017 Preliminaries)
PWG : PWG-CF (Flow and Correlations)
Energy: 2.76 TeV
System: Pb-Pb

Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]

Pion spectra comparison in real and measured spherocities

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

Real-measured spherocity correlation matrix in V0M 0-10% multiplicity events

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

pT-differential proton-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to Monte-Carlo

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

pT-differential kaon-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to Monte-Carlo

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

pT-differential proton yield in V0M 0-10%, high and low spherocities

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

pT-differential kaon yield in V0M 0-10%, high and low spherocities

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

pT-differential pion yield in V0M 0-10%, high and low spherocities

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

K*± in Inelastic pp Collisions at 5.02 TeV [IS17]

Ratios of pT spectra of K*± in minimum bias INEL pp collisions at 13 TeV to 5.02 TeV

Fig. Group : K*± in Inelastic pp Collisions at 5.02 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

K*± pT spectra

Fig. Group : K*± in Inelastic pp Collisions at 5.02 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

K*± vs K*0 pT spectra

Fig. Group : K*± in Inelastic pp Collisions at 5.02 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

D* jets in p-Pb 5 TeV (Run2)

Cross Section of Charged Jets (Anti-kT, R=0.4) Tagged with a D^{*} meson with $p_{\rm T,D} > 3 GeV/c$

Fig. Group : D* jets in p-Pb 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Reconstruction efficiency of D* in charged jets, p-Pb at 5.02 TeV (Run2)

Fig. Group : D* jets in p-Pb 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

D* in charged jets invariant mass distributions, D* pT intervals, p-Pb at 5.02 TeV (Run2)

Fig. Group : D* jets in p-Pb 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

D* in charged jets invariant mass distributions, jet pT intervals, p-Pb at 5.02 TeV (Run2)

Fig. Group : D* jets in p-Pb 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult

Heavy-flavour muon yield in pt bins vs. event multiplicity in pp collisions at 8 TeV: comparison with D meson measurements at 7 TeV

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 7 TeV, 8 TeV
System: p-p

y-differential cross section of muons from heavy flavour decays in pp collisions at 8 TeV (high pt)

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

y-differential cross section of muons from heavy flavour decays in pp collisions at 8 TeV (low pt)

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

y-differential cross section of muons from heavy flavour decays in pp collisions at 8 TeV

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

Ratio between data and FONLL calculations vs pt in different rapidity regions in pp collisions at 8 TeV

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

pt-differential cross sections of muons from heavy flavour decays in different rapidity regions in pp collisions at 8 TeV

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

pt-differential cross section of muons from heavy flavour decays in pp collisions at 8 TeV

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

Heavy-flavour muon yield in pt bins vs. event multiplicity in pp collisions at 8 TeV: comparison with EPOS predictions

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

Heavy-flavour muon yield in pt bins vs. event multiplicity in pp collisions at 8 TeV

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

Heavy-flavour muon yield vs. event multiplicity in pp collisions at 8 TeV

Fig. Group : Heavy-flavour muon production in pp collisions at 8 TeV and vs. mult
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)

Comparison of D-h away-side observables in p-Pb @ 5.02 TeV (2016) and from model predictions (higher pT ranges)

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Comparison of D-h away-side observables in p-Pb @ 5.02 TeV (2016) and from model predictions (lower pT ranges)

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Comparison of D-h near-side observables in p-Pb @ 5.02 TeV (2016) and from model predictions (higher pT ranges)

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Comparison of D-h near-side observables in p-Pb @ 5.02 TeV (2016) and from model predictions (lower pT ranges)

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Comparison of D-h correlation distributions in p-Pb @ 5.02 TeV (2016) and from model predictions (2/2)

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Comparison of D-h correlation distributions in p-Pb @ 5.02 TeV (2016) and from model predictions (1/2)

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Fit of D-h correlation distribution, for 5 < pT(D) < 8 GeV/c and pT(assoc) > 1 GeV/c, on p-Pb @ 5.02 TeV.

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Comparison of near-side observables from D-h correlations in pp @ 7 TeV and p-Pb @ 5.02 TeV (2016)

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Comparison of D-h correlation distributions in pp @ 7 TeV and p-Pb @ 5.02 TeV (2016)

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

D-h correlation distribution, for 5 < pT(D) < 8 GeV/c and pT(assoc) > 1 GeV/c, on p-Pb @ 5.02 TeV.

Fig. Group : D-h correlations in p-Pb @ 5.02 TeV (2016 data sample)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

SQM2017 (poster) Anisotropic azimuthal correlations of identified hadrons in p-Pb collisions at sqrt{s} = 5.02 TeV

v_2 of inclusive charged hadrons, K0s, Lambda and Phi in centrality 0-20% with published pi,K,p results from Run 1

Fig. Group : SQM2017 (poster) Anisotropic azimuthal correlations of identified hadrons in p-Pb collisions at sqrt{s} = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: p-Pb

v_2 of inclusive charged hadrons, K0s, Lambda and Phi in centrality 0-20%

Fig. Group : SQM2017 (poster) Anisotropic azimuthal correlations of identified hadrons in p-Pb collisions at sqrt{s} = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: p-Pb

Phi meson extraction method

Fig. Group : SQM2017 (poster) Anisotropic azimuthal correlations of identified hadrons in p-Pb collisions at sqrt{s} = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: p-Pb

Pb-Pb 5.02 TeV Run 2015

phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 0-10% and 60-90% centrality

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 0-10% and 10-20% centrality

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 0-10% and 40-60% centrality

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 60-90% centrality

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 40-60% centrality

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 20-40% centrality

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 10-20% centrality

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 0-10% centrality

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

phi Raa as a function of Npart in Pb-Pb collisions at 5.02 TeV

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Electrons from heavy-flavour hadron decays at mid-rapidity and low transverse momenta in pp collisions at sqrt(s) = 13 TeV

Electrons from heavy-flavour hadron decay cross section

Fig. Group : Electrons from heavy-flavour hadron decays at mid-rapidity and low transverse momenta in pp collisions at sqrt(s) = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Ratio inclusive over background electrons

Fig. Group : Electrons from heavy-flavour hadron decays at mid-rapidity and low transverse momenta in pp collisions at sqrt(s) = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Tagging Efficiency

Fig. Group : Electrons from heavy-flavour hadron decays at mid-rapidity and low transverse momenta in pp collisions at sqrt(s) = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Invariant mass

Fig. Group : Electrons from heavy-flavour hadron decays at mid-rapidity and low transverse momenta in pp collisions at sqrt(s) = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Fit of the TPC Nsigma

Fig. Group : Electrons from heavy-flavour hadron decays at mid-rapidity and low transverse momenta in pp collisions at sqrt(s) = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

(Anti-)Nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$=5.02 TeV and pp collisions at $\sqrt{s}$=13 TeV [SQM17]

Deuteron identification with TOF in pp at 13 TeV

Fig. Group : (Anti-)Nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$=5.02 TeV and pp collisions at $\sqrt{s}$=13 TeV [SQM17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

dbar to d ratio for pp collisions at 13 TeV

Fig. Group : (Anti-)Nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$=5.02 TeV and pp collisions at $\sqrt{s}$=13 TeV [SQM17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

Production of light flavor hadrons in pp collisions at 13 TeV [SQM17]

Ratios of transverse-momentum spectra of protons/antiprotons in minimum bias INEL pp collisions at various center-of-mass energies to 2.76 TeV

Fig. Group : Production of light flavor hadrons in pp collisions at 13 TeV [SQM17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 2.76 TeV, 5.02 TeV, 7 TeV, 13 TeV
System: p-p

Ratios of transverse-momentum spectra of charged pions in minimum bias INEL pp collisions at various center-of-mass energies to 2.76 TeV

Fig. Group : Production of light flavor hadrons in pp collisions at 13 TeV [SQM17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 2.76 TeV, 5.02 TeV, 7 TeV, 13 TeV
System: p-p

Transverse momentum spectra of light flavor hadrons measured at mid-rapidity in minimum bias inelastic pp collisions at 13 TeV

Fig. Group : Production of light flavor hadrons in pp collisions at 13 TeV [SQM17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

D meson in pp at 13 TeV (2016 data)

Ratio Dplus cross section in pp collisions at 13 TeV/ 7 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 7 TeV, 13 TeV
System: p-p

Ratio Dplus cross section in pp collisions at 13 TeV/ 5 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV, 13 TeV
System: p-p

Ratio D0 cross section in pp collisions at 13 TeV/ 5 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV, 13 TeV
System: p-p

Ratio D0 cross section in pp collisions at 13 TeV/ 7 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 7 TeV, 13 TeV
System: p-p

Ratio Dstar cross section in pp collisions at 13 TeV/ 5 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV, 13 TeV
System: p-p

Ratio Dstar cross section in pp collisions at 13 TeV/ 7 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 7 TeV, 13 TeV
System: p-p

D*+ invariant mass distribution in pp collisions at 13 TeV (pT [6,7] GeV/c)

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

D+ invariant mass distribution in pp collisions at 13 TeV (pT [24,36] GeV/c)

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

D+ reconstruction Efficiencies

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

D*+ reconstruction Efficiencies

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

D0 reconstruction Efficiencies

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV, 13 TeV
System: p-p

Ratio Dplus/D0 cross section in pp collisions at 13 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Ratio Dstar/Dplus cross section in pp collisions at 13 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Ratio Dstar/D0 cross section in pp collisions at 13 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Ratio Dplus cross section in pp collisions at 13 TeV/ 8 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV, 13 TeV
System: p-p

Ratio D0 cross section in pp collisions at 13 TeV/ 8 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV, 13 TeV
System: p-p

Ratio Dstar cross section in pp collisions at 13 TeV/ 8 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV, 13 TeV
System: p-p

Dplus cross section in pp collisions at 13 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

D0 cross section in pp collisions at 13 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Dstar cross section in pp collisions at 13 TeV

Fig. Group : D meson in pp at 13 TeV (2016 data)
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

D mesons in pp at 8 TeV

D0 reconstruction Efficiencies

Fig. Group : D mesons in pp at 8 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

D+ meson over D0 meson ratio in MB pp collisions at 8 TeV

Fig. Group : D mesons in pp at 8 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

D*+ meson over D0 meson ratio in MB pp collisions at 8 TeV

Fig. Group : D mesons in pp at 8 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

8 to 7 TeV ratio of the D0 meson production cross-sections

Fig. Group : D mesons in pp at 8 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

Dzero: Invariant mass (M(Kpi)) in 1-2, 5-6 and 16-24 GeV/c in pp at \sqrt{s} = 8 TeV

Fig. Group : D mesons in pp at 8 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

Cross-section of D0 meson in MB pp collisions at 8 TeV

Fig. Group : D mesons in pp at 8 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-p

K*± in Inelastic pp Collisions at 13 TeV [SQM17]

K*± /K and K*0/K vs. energy in different collision systems

Fig. Group : K*± in Inelastic pp Collisions at 13 TeV [SQM17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

Reconstruction Efficiency for K*± in pp collisions at 13 TeV

Fig. Group : K*± in Inelastic pp Collisions at 13 TeV [SQM17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

K*± signal after background subtraction

Fig. Group : K*± in Inelastic pp Collisions at 13 TeV [SQM17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p