Public Preliminary figures by analysis
Public Preliminary figures by analysis
Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 30 - 50% Centrality and pp
- Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: Pb-Pb
Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 0 - 10% Centrality and pp
- Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: Pb-Pb
Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 30 - 50% Centrality and pp
- Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: Pb-Pb
Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 0 - 10% Centrality and pp
- Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: Pb-Pb
Polarization of photoproduced J/psi in Pb-Pb (QM2023)
Comparison of $\lambda_{\theta}$ with UPC measurement
- Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System: Pb-Pb
dNdcostheta vs costheta in Pb--Pb collisions at 5.02 TeV using Helicity Frame
- Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System: Pb-Pb
Invariant mass distribution of dimuon pairs for 0.5 < |cos\theta| < 0.6 in Pb-Pb collsions at 5.02 TeV
- Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System: Pb-Pb
Invariant mass distribution of dimuon pairs for 0.2 < |cos\theta| < 0.3 in Pb-Pb collsions at 5.02 TeV
- Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System: Pb-Pb
Invariant mass distribution of dimuon pairs for 0.0 < |cos\theta| < 0.1 in Pb-Pb collsions at 5.02 TeV
- Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System: Pb-Pb
$\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV
BR ratio comparisons
- Fig. Group : $\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
The measurements of the $\Omega_{\rm c}^{0}-$baryon, not corrected by the BRs, in the two different decay channels (hadronic and semileptonic), also the ratio of the branching fraction
- Fig. Group : $\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Acceptance and efficiency of $\Omega_{\rm c}^{0} \rightarrow e^{+}\Omega^{-}\nu_{e}$
- Fig. Group : $\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Response matrix
- Fig. Group : $\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Invariant mass distribution of $e\Omega$
- Fig. Group : $\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
[EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
Rg vs pt (HM)
- Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 13 TeV
- System: p-p
Rg vs pt (MB)
- Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 13 TeV
- System: p-p
Photon yield vs multiplicity (pp13TeV)
- Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 13 TeV
- System: p-p
Direct photon pt (HM)
- Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 13 TeV
- System: p-p
Direct photon pt (MB)
- Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 13 TeV
- System: p-p
r vs pt HM (updated)
- Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 13 TeV
- System: p-p
r vs pt MB (updated)
- Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 13 TeV
- System: p-p
Upsilon cross section in pp collisions at 13 TeV (HP2023)
y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to ICEM+FONLL
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to ICEM+FONLL
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
Integrated Upsilon(1S) and Upsilon(2S) cross section as a function of energy compared to ICEM+FONLL model calculations
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to LHCb
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
y-differential upsilon(1S) pp cross section at 13 TeV compared to lower energy ALICE data
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to LHCb
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
pT differential Upsilon(1S) and Upsilon(2S) cross section in pp collisions at 13 TeV
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
pT differential Upsilon(1S) cross section in pp collisions at 13 TeV compared to lower energy ALICE data
- Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
Hardest kt splittings in pp and PbPb at 5 TeV
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - soft drop zcut = 0.2, comparison with models
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - soft drop zcut = 0.4, comparison with models
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - soft drop zcut = 0.2, comparison with models
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - Dynamical grooming a = 1.0 z > 0.2, comparison with models
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - Dynamical grooming a = 1.0, comparison with models
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - additional grooming methods comparison with PYTHIA8
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - selection of grooming methods
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - additional grooming methods
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - selection of grooming methods
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - additional grooming methods
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - original grooming methods
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - selection of grooming methods
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - additional grooming methods
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Soft Drop z_cut = 0.4
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 2.0, z > 0.2
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 1.0, z > 0.2
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 0.5, z > 0.2
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Soft Drop z_cut = 0.2
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 2.0
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 1.0
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 0.5
- Fig. Group : Hardest kt splittings in pp and PbPb at 5 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=3$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=2$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=1.5$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=1$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
Feed-down fraction in D$^{0}$-tagged jet angularity in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 5 < $p_{\rm T,D^{0}}$ < 20 GeV/c for R = 0.4, $\alpha=1$.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=3$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=2$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=1.5$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
D0-tagged jet raw angularity distributions for $\alpha=1$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 8 < $p_{\rm T,D^{0}}$ < 12 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
Invariant mass distribution of D$^{0}$-tagged jet candidates with 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 8 < $p_{\rm T,D^{0}}$ < 12 GeV/c for R = 0.4.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=1$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.
- Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p
Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV
EEC distribution for 40-60GeV 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
Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
Away-Side width comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Away-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Away-Side yields and widths comparison between measured Λc-h and PYTHIA8 predictions
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Near-Side width comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Near-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Near-Side yields and widths comparison between measured Λc-h and PYTHIA8 predictions
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Away-Side Width comparison between Λc-h and D-h at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Away-Side Yield comparison between Λc-h and D-h at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Away-Side yields and widths comparison between Λc-h and D-h
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Baseline comparison between Λc-h and D-h at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Near-Side width comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Near-Side Yield comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Near-Side yields and widths comparison between Λc-h and D-h
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Comparison between measured Λc+-h and D-h azimuthal correlation distributions
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Comparison between the measured Λc-h azimuthal correlation distributions and PYTHIA8 predictions at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Comparison between the measured Λc-h azimuthal correlation distributions and PYTHIA8 predictions
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Comparison between Λc-h and D-h azimuthal correlation distributions measured in the transverse momentum interval 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c
- Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
Non-prompt $\rm D^{+}$ production cross section in pp collisions at 13 TeV vs. models
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D_{s}^{+}$ production cross section in pp collisions at 13 TeV vs. models
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D^{+}$/$\rm D^{0}$ ratio in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D_{s}^{+}$/$\rm D^{0}$ ratio in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D_{s}^{+}$/$\rm D^{+}$ ratio in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D_{s}^{+}$/($\rm D^{+}$ + $\rm D^{0}$) ratio in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
$\rm D^{+}$ efficiency times acceptance in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
$\rm D_{s}^{+}$ efficiency times acceptance in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D^{+}$ cut variation in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D_{s}^{+}$ cut variation in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D^{0}$, $\rm D^{+}$, $\rm D_{s}^{+}$ fraction pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D^{+}$ invariant-mass distribution in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-prompt $\rm D_{s}^{+}$ invariant-mass distribution in pp collisions at 13 TeV
- Fig. Group : Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Charm production cross section and fragmentation fractions in p-Pb
Integrated $R_\mathrm{pPb}$ of charm, D$^{0}$, $\Lambda_\mathrm{c}^{+}$ and J/$\psi$
- Fig. Group : Charm production cross section and fragmentation fractions in p-Pb
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.02 TeV
- System: p-p, p-Pb
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, 5.02 TeV, 7 TeV
- System: p-p, 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, p-Pb
Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE
$p_{\rm T}$-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
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