| $\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons in $0.3<|y|<0.8$ with respect to the reaction plane and a random axis in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
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| $\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons with $15<p_\mathrm{T}<30$ GeV$/c$ with respect to the reaction and production planes in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
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| $\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons with $15<p_\mathrm{T}<30$ GeV$/c$ as a function of $|y|$ with respect to the reaction plane in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
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| $\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons in $0.3<|y|<0.8$ with respect to the reaction plane in 0-10% and 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
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| Non-prompt fraction of $\mathrm{D}^{*+}$ candidates in 0-10% and 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
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| $|\cos{\vartheta^*}|$ differential corrected yields of $\mathrm{D}^{*+}$ candidates in two $p_\mathrm{T}$ intervals, for $0.3<|y|<0.8$ in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
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| Invariant-mass distributions of $\mathrm{D}^{*+}$ candidates in two $p_\mathrm{T}$ and $|\cos{\vartheta^*}|$ intervals, for $0.3<|y|<0.8$ in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
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| Direct photon pt (MB and HM)
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| $\rm D^{0}$-tagged raw jet axis distribution, $\Delta R_{\rm STD,D}$, for $R = 0.4$ in $10 < p_{\rm T,ch~ jet} < 20 {\rm ~ GeV}/c$
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| Fully corrected $\rm D^{0}$-tagged jet axis distribution, $\Delta R_{\rm STD,D}$, compared to PYTHIA 8 for $R = 0.4$ in $10 < p_{\rm T,ch~ jet} < 20 {\rm ~ GeV}/c$
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| Feed-down fraction in $\rm D^{0}$-tagged jet axis difference, $\Delta R_{\rm STD,D}$, in $10 < p_{\rm T, ch ~ jet} < 20 ~ {\rm GeV}/c$ and $5 < p_{\rm T, D^{0}} < 20 ~ {\rm GeV}/c$ for $R=0.4$.
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| Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 30 - 50% Centrality and pp
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| Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp
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| Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 30 - 50% Centrality
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| Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10% Centrality
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| Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 30 - 50% Centrality
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| Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality
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| Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 30 - 50% Centrality
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| Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality
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| Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 30 - 50% Centrality and pp
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| Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 0 - 10% Centrality and pp
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| Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 30 - 50% Centrality and pp
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| Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 0 - 10% Centrality and pp
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| Comparison of $\lambda_{\theta}$ with UPC measurement
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| dNdcostheta vs costheta in Pb--Pb collisions at 5.02 TeV using Helicity Frame
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| Invariant mass distribution of dimuon pairs for 0.5 < |cos\theta| < 0.6 in Pb-Pb collsions at 5.02 TeV
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| Invariant mass distribution of dimuon pairs for 0.2 < |cos\theta| < 0.3 in Pb-Pb collsions at 5.02 TeV
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| Invariant mass distribution of dimuon pairs for 0.0 < |cos\theta| < 0.1 in Pb-Pb collsions at 5.02 TeV
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| BR ratio comparisons
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| 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
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| Acceptance and efficiency of $\Omega_{\rm c}^{0} \rightarrow e^{+}\Omega^{-}\nu_{e}$
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| Response matrix
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| Invariant mass distribution of $e\Omega$
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| Rg vs pt (HM)
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| Rg vs pt (MB)
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| Photon yield vs multiplicity (pp13TeV)
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| Direct photon pt (HM)
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| Direct photon pt (MB)
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| r vs pt HM (updated)
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| r vs pt MB (updated)
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| y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to ICEM+FONLL
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| pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to ICEM+FONLL
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| Integrated Upsilon(1S) and Upsilon(2S) cross section as a function of energy compared to ICEM+FONLL model calculations
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| pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to LHCb
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| y-differential upsilon(1S) pp cross section at 13 TeV compared to lower energy ALICE data
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| y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to LHCb
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| y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV
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| pT differential Upsilon(1S) and Upsilon(2S) cross section in pp collisions at 13 TeV
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| pT differential Upsilon(1S) cross section in pp collisions at 13 TeV compared to lower energy ALICE data
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - soft drop zcut = 0.2, comparison with models
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - soft drop zcut = 0.4, comparison with models
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - soft drop zcut = 0.2, comparison with models
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| 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
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - Dynamical grooming a = 1.0, comparison with models
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - additional grooming methods comparison with PYTHIA8
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - selection of grooming methods
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - additional grooming methods
|
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - selection of grooming methods
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - additional grooming methods
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - original grooming methods
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - selection of grooming methods
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - additional grooming methods
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|
| 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.
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| 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.
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| 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.
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| 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.
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| EEC distribution for 40-60GeV charged jets in pp collision (theory comparison included)
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| 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, $\alpha=1$.
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| 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.
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| 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.
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| 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.
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| 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.
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| 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.
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|
| 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
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 2.0
|
|
| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 1.0
|
|
| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 0.5
|
|
| Away-Side width comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
|
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| Away-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
|
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| Away-Side yields and widths comparison between measured Λc-h and PYTHIA8 predictions
|
|
| Near-Side width comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
|
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| Near-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
|
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| Near-Side yields and widths comparison between measured Λc-h and PYTHIA8 predictions
|
|
| 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
|
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| 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
|
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| Away-Side yields and widths comparison between Λc-h and D-h
|
|
| Baseline comparison between Λc-h and D-h at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c
|
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| Near-Side width comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c
|
|
| Near-Side Yield comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c
|
|
| Near-Side yields and widths comparison between Λc-h and D-h
|
|
| Comparison between measured Λc+-h and D-h azimuthal correlation distributions
|
|
| 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
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| Comparison between the measured Λc-h azimuthal correlation distributions and PYTHIA8 predictions
|
|
| 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
|
|
| 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.
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| Integrated $R_\mathrm{pPb}$ of charm, D$^{0}$, $\Lambda_\mathrm{c}^{+}$ and J/$\psi$
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