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J/ψ v2{SP} vs centrality at forward rapidity in the dimuon channel for 5 < pT < 20 GeV/c and at 5.36 TeV Fig. Group : Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ v2{SP} vs centrality at forward rapidity in the dimuon channel for pT < 5 GeV/c and at 5.36 TeV Fig. Group : Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Prompt/non-prompt $J/\psi$ fraction at forward rapidity as a function of $p_{T}$ Fig. Group : Prompt/non-prompt J/$\psi$ separation at foward rapidity in pp collisions at 13.6 TeV PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 0-10% and at 5.36 TeV Fig. Group : Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 30-50% and at 5.36 TeV Fig. Group : Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV Fig. Group : Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
ϒ(1S) v2 calculation at fwd rapidity for the centality class 5-60%, pT class 0-3 GeV/c at 5.36 TeV, with the v2 background parametrized by the Chebyshev function Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
ϒ(1S) v2 calculation at fwd rapidity for the centality class 5-60%, pT class 0-3 GeV/c at 5.36 TeV, with the v2 background parametrized by Pol2 Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Cut variation of $\Lambda_c$ in pt 2 to 3 geV/c in pp collisions at 13.6 TeV Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
p-$\Lambda_c$ inv.mass in mixed-event in pp collisions at 13.6 TeV Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
p-$\Lambda_c$ inv.mass in same-event in pp collisions at 13.6 TeV Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
p-$\Lambda_c$ raw correlation function compare with models included strong interaction in pp collisions at 13.6 TeV Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
p-$\Lambda_c$ raw correlation function fit decomposition in pp collisions at 13.6 TeV Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
p-$\Lambda_c$ raw correlation function fit with coulomb only and background in pp collisions at 13.6 TeV Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Ds1+/Ds ratio, (BR factorized) Fig. Group : Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Ds2/Ds ratio, (BR factorized) Fig. Group :** Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Ds2/Ds ratio Fig. Group :** Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Ds1+/Ds ratio Fig. Group : Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Ds, Ds1+ and Ds2 cross section Fig. Group :** Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Ds1+ Invariant Mass 2<pT<3 GeV/c Fig. Group : Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Ds1+ Invariant Mass 6<pT<8 GeV/c Fig. Group : Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Ds1+ Invariant Mass 12<pT<24 GeV/c Fig. Group : Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Ds2 Invariant Mass 12<pT<24 GeV/c Fig. Group :** Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Ds2 Invariant Mass 6<pT<8 GeV/c Fig. Group :** Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Ds2 Invariant Mass 2<pT<4 GeV/c Fig. Group :** Ds1+and Ds2+ production in pp collisions at 13.6 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between CMS and ALICE for the Y(1S) v2 as a function of pT at fwd rapidity for the centality class 5-60% at 5.36 TeV Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.02 TeV , Energy: 5.36 TeV System Pb-Pb
Comparison between the Blast wave description and Run 3 for the Y(1S) v2 as a function of pT at fwd rapidity for the centality class 5-60% at 5.36 TeV Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Comparison between models (TAMU and BBJS) and Run 3 for the Y(1S) v2 as a function of pT at fwd rapidity for the centality class 5-60% at 5.36 TeV Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Comparison between Run2 and Run 3 for the Y(1S) v2 as a function of centrality at fwd rapidity for the pT range 2-15 GeV/c Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.02 TeV , Energy: 5.36 TeV System Pb-Pb
Y(1S) v2 as a function of centrality at fwd rapidity for the pT range 2-15 GeV/c at 5.36 TeV Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Comparison between Run2 and Run 3 for the Y(1S) v2 as a function of pT at fwd rapidity for the centality class 5-60% Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.02 TeV , Energy: 5.36 TeV System Pb-Pb
Y(1S) v2 as a function of pT at fwd rapidity for the centality class 5-60% at 5.36 TeV Fig. Group : Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Longitudinal polarization ($P_{\rm z}$) of prompt and non-prompt $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame) Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Longitudinal polarization as a function of non-prompt fraction for $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame) Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Simultaneous fit of $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ corrected yield as a function of $\cos(\theta^)$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame) Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System** p-p
*Invariant mass distribution of ${\rm pK}\pi$ triplets in pp collisions at $\sqrt{s} = 13.6$ TeV in two intervals of $\cos(\theta^)$ (production frame) Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System** p-p
Ratio of the $R_{\rm T}$-dependent per-event D$^0$ meson yields to the $R_{\rm T}$-integrated yield in the toward region Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Acceptance-times-efficiency correction of D$^0$ mesons as a function of the $R_{\rm T}$ Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Invariant mass distribution of D$^0$ candidates with 12 < $p_{\rm T}^{\rm D^0}$ < 18 GeV/$c$ in $R_{\rm T}$ > 1 events Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Invariant mass distribution of D$^0$ candidates with 5 < $p_{\rm T}^{\rm D^0}$ < 8 GeV/$c$ in $R_{\rm T}$ < 1 events Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Inclusive charged-particle jet invariant yield in pp collisions at \sqrt{s} = 13.6 TeV Fig. Group : Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV Fig. Group : Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
p/pi in jets 3 curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
K/pi in jets 3 curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
pi spectra inclusive, jet+UE, UE Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
pi spectra inclusive and jet+UE Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
pi spectra inclusive only Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
p/pi in jets all 5 curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
K/pi in jets all 5 curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
p in jets spectra Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
K in jets spectra Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
pi in jets spectra - all four curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
nSD of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
nSD of D0-tagged jets in pp at 13.6 TeV Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
$\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
zg of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
zg of D0-tagged jets in pp at 13.6 TeV Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
$\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV vs $\text{D}^{0}$ Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
$\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV with PYTHIA comparison Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV, just Run 3 data Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Raw spectra of signal, reference and delta recoil vs pT for R=0.4 jets Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Delta recoil vs pT with PYTHIA comparison for R=0.4 jets in 13.6 TeV pp collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Delta recoil vs pT with PYTHIA comparison for R=0.2 jets in 13.6 TeV pp collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Delta recoil vs pT for R=0.4 jets in 13.6 TeV pp collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Delta recoil vs pT for R=0.2 jets in 13.6 TeV pp collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Evolution of power index as a function of $\it{p}_{\rm{T}}$ Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Normalized $\it{p}_{\rm{T}}$ correlator as a function of mean $\it{p}_{\rm{T}}$ for fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$ Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Normalized $\it{p}_{\rm{T}}$ correlator as a function of mean $\it{p}_{\rm{T}}$ with increasing upper limit of $\it{p}_{\rm{T}}$ windows Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Relative uncertainties of inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV Fig. Group : Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Comparison of Pythia8 (Monash) and EPOS models to normalized mean $\it{p}_{\rm{T}}$ correlator as charged particle multiplicity at fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$ Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Comparison of Pythia8 (Monash) and EPOS models to normalized mean $\it{p}_{\rm{T}}$ correlator as charged particle multiplicity for increasing upper limit of $\it{p}_{\rm{T}}$ windows Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Empirical power law fit to normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity for fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$ Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity with increasing upper limit of $\it{p}_{\rm{T}}$ windows Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Mean $\it{p}_{\rm{T}}$ as a function of charged particle multiplicity at fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$ Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Mean $\it{p}_{\rm{T}}$ as a function of charged particle multiplicity for increasing upper limit of $\it{p}_{\rm{T}}$ windows Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges PWG : PWG-CF (Flow and Correlations) Energy: 13 TeV System p-p
Ratio of zg distribution for wide and narrow jets in pp and Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Ratio of θg distribution for balanced and unbalanced jets in pp and Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
zg distribution for wide jets in pp and Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
zg distribution for narrow jets in pp and Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
θg distribution for balanced jets in pp and Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
θg distribution for unbalanced jets in pp and Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
zg distribution for wide jets in Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
zg distribution for narrow jets in Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
θg distribution for balanced jets in Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
θg distribution for unbalanced jets in Pb-Pb Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
zg distribution for wide jets in pp Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p

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