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ID number ALI-PREL-XXX

Figure Caption

Scope: PWG

System

Energy

Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity

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

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

Prompt/non-prompt J/$\psi$ separation at foward rapidity in pp collisions at 13.6 TeV

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

Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity

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

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, 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, 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, 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

p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV

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+and Ds2*+ production in pp collisions at 13.6 TeV

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

$\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV

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

D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV

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 cross section in pp collisions at \sqrt{s} = 13.6 TeV

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

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

pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary

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

Substructure of charm-tagged jets in pp collisions at 13.6 TeV

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

Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data

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

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

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

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 $\it{p}_{\rm{T}}$