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Total charm production cross section in pp and p-Pb collisions as a function of $\sqrt{s}$ Fig. Group : Charm production cross section and fragmentation fractions in p-Pb PWG : PWG-HF (Heavy Flavour) Energy: 2.76 TeV , Energy: 5.02 TeV , Energy: 7 TeV System p-p , System p-Pb
$p_{\rm T}$-integrated non-prompt $\rm D^{0}$ $R_{\rm pPb}$ from 0-24 GeV/$\it{c}$ in pPb collisions at 5.02 TeV Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Charm-hadron fragmentation fractions in pp and p-Pb collisions including measured Xic in p-Pb (2023) Fig. Group : Charm production cross section and fragmentation fractions in p-Pb PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-p , System p-Pb
Invariant-mass distribution of non-prompt $\rm D^{0}$ in pPb collisions at 5.02 TeV Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV compared with CMS measurement in log scale Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV compared with CMS measurement Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
$p_{\rm T}$-integrated non-prompt $\rm D^{0}$ $R_{\rm pPb}$ from 2-24 GeV/$\it{c}$ in pPb collisions at 5.02 TeV Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Non-prompt $\rm D^{0}$ fractions Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$ Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Non-prompt $\rm D^{0}$ / non-prompt $\Lambda_{\rm c}^{+}$ in pPb collisions at 5.02 TeV Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Contributions of prompt and non-prompt $\rm D^{0}$ estimated with the cut-variation method Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$ Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Production cross section of non-prompt $\rm D^0$ production in p-Pb collisions at 5.02 TeV Fig. Group : Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
$\Xi_c^0$/$\Lambda_c^+$ production cross section ratio as a function of 𝑝T in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV Fig. Group : Measurement of $\Xi_c^0$ production in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
$\Xi_c^0$/$D^0$ production cross section ratio as a function of 𝑝T in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV Fig. Group : Measurement of $\Xi_c^0$ production in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Nuclear modification factor of the $\Xi_c^0$ baryon in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV Fig. Group : Measurement of $\Xi_c^0$ production in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Acceptance x efficiency as a function of 𝑝T for $\Xi_c^0$ baryons Fig. Group : Measurement of $\Xi_c^0$ production in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Invariant-mass distribution of $\Xi_c^0$ in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV Fig. Group : Measurement of $\Xi_c^0$ production in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
$\Xi_c^0$ baryon production cross section in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV Fig. Group : Measurement of $\Xi_c^0$ production in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System p-Pb
Response matrix for R=0.3 jets in central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Corrected jet $p_{T,jet}$ distribution with $p_{T}^{lead} > 5$ GeV/c for central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Raw correlated inclusive jet $p_{T,jet}^{reco}$ distribution for central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 5$ GeV/c for central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Raw inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME for central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 5$ GeV/c for central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Invariant Cross-Section Ratios of Different Jet Radii for pp Full Jet Spectra 8 TeV with Comparison to PYTHIA8 Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
Fragmentation function of J/psi-tagged charged jets Fig. Group : J/psi production in jets at midrapidity in pp collisions at 13 TeV (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
Fragmentation function of non-prompt J/psi-tagged charged jets Fig. Group : J/psi production in jets at midrapidity in pp collisions at 13 TeV (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
Fragmentation function of prompt J/psi-tagged charged jets Fig. Group : J/psi production in jets at midrapidity in pp collisions at 13 TeV (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
f_B signal extraction 0.7 < z < 0.8 Fig. Group : J/psi production in jets at midrapidity in pp collisions at 13 TeV (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
Inclusive jpsi signal extraction, 0.7 < z < 0.8 Fig. Group : J/psi production in jets at midrapidity in pp collisions at 13 TeV (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
Fiducial cross section of Z->ee at mirapidity in pp collisions at 13 TeV Fig. Group : Z→e+e− in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Invariant mass of Z->ee (ULS and LS pairs) at midrapidity in pp collisions at 13 TeV Fig. Group : Z→e+e− in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Invariant mass of Z->ee at midrapidity in pp collisions at 13 TeV Fig. Group : Z→e+e− in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
The comparison of longitudinal momentum fraction of $\rm D_{s}^{+}$ and $\rm D^{0}$ -tagged jets in MB pp collisions at 13 TeV Fig. Group : Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Longitudinal momentum fraction of $\rm D_{s}^{+}$-tagged jets in MB pp collisions at 13 TeV Fig. Group : Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Relative statistical and systematic uncertainties by categories of $\rm D_{s}^{+}$-tagged jets longitudinal momentum fraction in MB pp collisions at 13 TeV Fig. Group : Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Feed-down contribution of $\rm D_{s}^{+}$ jets from POWHEG+PYTHIA6+EvtGen in MB pp collisions at 13 TeV Fig. Group : Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Invariant mass distribution of $\rm D_{s}^{+}$ candidates inside jets in MB pp collisions at 13 TeV Fig. Group : Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
*$\mathrm{D_{s2}^{+}} /\mathrm{D_{s}^{+}} $ corrected-yield ratio vs multiplicity Fig. Group :** Measurement of $\mathrm{D_{s1}^{+}}$ and $\mathrm{D_{s2}^{+}}$ mesons in pp collisions at $\sqrt{s} = 13$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
$\mathrm{D_{s1}^{+}} /\mathrm{D_{s}^{+}} $ corrected-yield ratio vs multiplicity Fig. Group : Measurement of $\mathrm{D_{s1}^{+}}$ and $\mathrm{D_{s2}^{+}}$ mesons in pp collisions at $\sqrt{s} = 13$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
*$\mathrm{D_{s1}^{+}}$-, $\mathrm{D_{s2}^{+}}$-, and $\mathrm{D_{s}^{+}}$-meson corrected yields vs multiplicity Fig. Group :** Measurement of $\mathrm{D_{s1}^{+}}$ and $\mathrm{D_{s2}^{+}}$ mesons in pp collisions at $\sqrt{s} = 13$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
*Invariant-mass distribution of $\mathrm{D_{s2}^{+}}$ mesons in HM pp collisions at 13 TeV Fig. Group :** Measurement of $\mathrm{D_{s1}^{+}}$ and $\mathrm{D_{s2}^{+}}$ mesons in pp collisions at $\sqrt{s} = 13$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
*Invariant-mass distribution of $\mathrm{D_{s2}^{+}}$ mesons in MB pp collisions at 13 TeV Fig. Group :** Measurement of $\mathrm{D_{s1}^{+}}$ and $\mathrm{D_{s2}^{+}}$ mesons in pp collisions at $\sqrt{s} = 13$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Invariant-mass distribution of $\mathrm{D_{s1}^{+}}$ mesons in HM pp collisions at 13 TeV Fig. Group : Measurement of $\mathrm{D_{s1}^{+}}$ and $\mathrm{D_{s2}^{+}}$ mesons in pp collisions at $\sqrt{s} = 13$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Invariant-mass distribution of $\mathrm{D_{s1}^{+}}$ mesons in MB pp collisions at 13 TeV Fig. Group : Measurement of $\mathrm{D_{s1}^{+}}$ and $\mathrm{D_{s2}^{+}}$ mesons in pp collisions at $\sqrt{s} = 13$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
EEC distribution for 60-80GeV charged jets in pp collision (theory comparison included) Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distribution for 20-40GeV charged jets in pp collision (theory comparison included) Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distributions of charged jets in Herwig pp events -- x (R_{L}) axis scaled by average charged jet pt, y axis divided by bin width and random normalized to focus on shape Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distributions of charged jets in Pythia pp events -- x (R_{L}) axis scaled by average charged jet pt, y axis divided by bin width and random normalized to focus on shape Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distributions of charged jets in pp collision -- x (R_{L}) axis scaled by average charged jet pt, y axis divided by bin width and random normalized to focus on shape Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distributions of charged jets in pp collision -- x (R_{L}) axis scaled by average charged jet pt, y axis not divided by bin width Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distributions of charged jets in pp collision -- x (R_{L}) axis scaled by average charged jet pt, y axis divided by bin width Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distribution charged jets in pp collision -- different jet pt comparison (20-40, 40-60, 60-80GeV), y axis divided by bin width Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distributions of charged jets in pp collision -- different jet pt comparison (20-40, 40-60, 60-80GeV), y axis not divided by bin width Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distribution for 60-80GeV charged jets in pp collision (model comparison included) Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distribution for 40-60GeV charged jets in pp collision (model comparison included) Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC distribution for 20-40GeV charged jets in pp collision (model comparison included) Fig. Group : Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Energy flow distributions overview Charged jets 60-80 GeV pp 13 TeV, R=0.05 to 0.1, R=0.2 to 0.25 and R=0.35 to 0.4 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions overview Charged jets 40-60 GeV pp 13 TeV, R=0.05 to 0.1, R=0.2 to 0.25 and R=0.35 to 0.4 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions overview Charged jets 60-80 GeV pp 13 TeV, All Rjet pairs Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions overview Charged jets 40-60 GeV pp 13 TeV, All Rjet pairs Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.35 to R=0.4 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.35 to R=0.4 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.2 to R=0.25 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.2 to R=0.25 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.05 to R=0.1 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.05 to R=0.1 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Mean energy flow versus jet radius with model comparison Charged jets 60-80 GeV pp 13 TeV Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Mean energy flow versus jet radius with model comparison Charged jets 40-60 GeV pp 13 TeV Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Mean energy flow versus jet radius with jet pt dependence Charged jets pp 13 TeV Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Measured $j_\mathrm{T}$ distributions in high $z$ bin compared to PYTHIA8 Tune4C Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Measured $j_\mathrm{T}$ distributions in mid $z$ bin compared to PYTHIA8 Tune4C Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Measured $j_\mathrm{T}$ distributions in low $z$ bin compared to PYTHIA8 Tune4C Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Measured $j_\mathrm{T}$ distributions in inclusive $z$ bin compared to PYTHIA8 Tune4C Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Measured $j_\mathrm{T}$ distributions in high $z$ bin compared to Herwig Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Measured $j_\mathrm{T}$ distributions in mid $z$ bin compared to Herwig Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Measured $j_\mathrm{T}$ distributions in low $z$ bin compared to Herwig Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Measured $j_\mathrm{T}$ distributions in inclusive $z$ bin compared to Herwig Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
[HP 2023] Beauty cross section as a function of rapidity compared with FONLL prediction (NNPDF pdf) Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
[HP 2023] Beauty cross section as a function of rapidity compared with FONLL prediction (CTEQ6 pdf) Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
[HP 2023] Charm cross section as a function of rapidity compared with FONLL prediction (CTEQ6 pdf) Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
[HP 2023] Charm cross section as a function of rapidity compared with FONLL prediction (NNPDF pdf) Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
[HP 2023] Simultaneous unbinned fit to dimuon data distribution (transverse momentum component) Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
[HP 2023] Simultaneous unbinned fit to dimuon data distribution (mass component) Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
[HP 2023] Dimuon invariant mass distribution with m>4 Gev/c^2 Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13 TeV System p-p
Experimental and theoretical uncertainties of the isolated prompt photon $R_{pA}$ at $\sqrt{s_{NN}}=8.16$ TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p , System p-Pb
Isolated prompt photon purity in p-Pb collisions at 8.16 TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-Pb
Data/theory ratio of isolated prompt photon production in p-Pb collisions at 8.16 TeV compared to p-Pb data at 5.02 TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV , Energy: 8 TeV System p-Pb
Isolated prompt photon production cross section in pp and p-Pb collisions at 8.16 TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p , System p-Pb
Nuclear modification factor of isolated prompt photon production in p-Pb collisions at 8.16 TeV (log x) Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p , System p-Pb
Nuclear modification factor of isolated prompt photon production in p-Pb collisions at 8.16 TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p , System p-Pb
Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.5 Full Jets in pp to PYTHIA8 Monash Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.4 Full Jets in pp to PYTHIA8 Monash Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.3 Full Jets in pp to PYTHIA8 Monash Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
Comparison of the Invariant Cross-Section for R = 0.5 Full Jets in pp to PYTHIA8 Monash Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
Comparison of the Invariant Cross-Section for R = 0.4 Full Jets in pp to PYTHIA8 Monash Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
Comparison of the Invariant Cross-Section for R = 0.3 Full Jets in pp to PYTHIA8 Monash Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
Comparison of the Invariant Cross-Section for R = 0.2 Full Jets in pp to PYTHIA8 Monash Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p

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