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ID number ALI-PREL-XXX

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Away-side yield comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Away-side width comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Near-side width comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between measured Ds-h and D+-h azimuthal correlation distributions (5 < $p_{T}$ < 8 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between measured Ds-h and D+-h azimuthal correlation distributions (3 < $p_{T}$ < 5 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (1 < $p_{T}$ < 3 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (3 < $p_{T}$ < 5 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (5 < $p_{T}$ < 8 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (8 < $p_{T}$ < 16 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (16 < $p_{T}$ < 36 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
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
Ratio of EECs in p-Pb and pp in different jet pT bins (20-27, 27-40, 40-80 GeV) Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-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
Ratio of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c with fit Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
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
Ratio of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c with HT calculation Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Ratio of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c with model+nPDF bands Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
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
Ratio of EECs in p-Pb/pp for 60-80 GeV/c jets Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Ratio of EECs in p-Pb/pp for 40-60 GeV/c jets Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Ratio of EECs in p-Pb/pp for 20-40 GeV/c jets Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Fitted EEC peak heights in p-Pb Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Fitted EEC peak positions in p-Pb Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Fit of EECs for 60-80 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Fit of EECs for 40-60 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Fit of EECs for 20-40 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Ratio of EECs in p-Pb/pp for 60-80 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV) Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Ratio of EECs in p-Pb/pp for 40-60 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV) Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 60-80 GeV/c jets Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 40-60 GeV/c jets Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 20-40 GeV/c jets Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 60-80 GeV/c Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 40-60 GeV/c Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
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

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