| 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
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| 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
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| 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
|
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| 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
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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 = 0.2
|
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 2.0
|
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 1.0
|
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| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 0.5
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| 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
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| 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
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| 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
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| 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
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| Near-Side Yield comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c
|
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| Near-Side yields and widths comparison between Λc-h and D-h
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| Comparison between measured Λc+-h and D-h azimuthal correlation distributions
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| 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
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| 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
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| Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=1$, $R=0.4$ 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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| Total charm production cross section in pp and p-Pb collisions as a function of $\sqrt{s}$
|
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| $p_{\rm T}$-integrated non-prompt $\rm D^{0}$ $R_{\rm pPb}$ from 0-24 GeV/$\it{c}$ in pPb collisions at 5.02 TeV
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| Charm-hadron fragmentation fractions in pp and p-Pb collisions including measured Xic in p-Pb (2023)
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| Invariant-mass distribution of non-prompt $\rm D^{0}$ in pPb collisions at 5.02 TeV
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| Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV compared with CMS measurement in log scale
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| Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV compared with CMS measurement
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| $p_{\rm T}$-integrated non-prompt $\rm D^{0}$ $R_{\rm pPb}$ from 2-24 GeV/$\it{c}$ in pPb collisions at 5.02 TeV
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| Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV
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| Non-prompt $\rm D^{0}$ fractions
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| Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
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| Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
|
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| Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
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| Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
|
|
| Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
|
|
| Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
|
|
| Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$
|
|
| 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 $R=0.2$
|
|
| Non-prompt $\rm D^{0}$ / non-prompt $\Lambda_{\rm c}^{+}$ in pPb collisions at 5.02 TeV
|
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| Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
|
|
| Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
|
|
| Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$
|
|
| Measurement of the ungroomed 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 $R=0.2$
|
|
| Contributions of prompt and non-prompt $\rm D^{0}$ estimated with the cut-variation method
|
|
| Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
|
|
| Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
|
|
| 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 $R=0.2$
|
|
| Production cross section of non-prompt $\rm D^0$ production in p-Pb collisions at 5.02 TeV
|
|
| $\Xi_c^0$/$\Lambda_c^+$ production cross section ratio as a function of 𝑝T in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
|
|
| Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
|
|
| $\Xi_c^0$/$D^0$ production cross section ratio as a function of 𝑝T in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
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|
| Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
|
|
| Nuclear modification factor of the $\Xi_c^0$ baryon in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
|
|
| Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
|
|
| Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
|
|
| Acceptance x efficiency as a function of 𝑝T for $\Xi_c^0$ baryons
|
|
| Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
|
|
| Invariant-mass distribution of $\Xi_c^0$ in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
|
|
| $\Xi_c^0$ baryon production cross section in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
|
|
| Corrected jet $p_{T,jet}$ distribution with $p_{T}^{lead} > 5$ GeV/c for central Pb-Pb collisions at 5.02 TeV
|
|
| Raw correlated inclusive jet $p_{T,jet}^{reco}$ distribution for central Pb-Pb collisions at 5.02 TeV
|
|
| 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
|
|
| Raw inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME for central Pb-Pb collisions at 5.02 TeV
|
|
| 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
|
|
| Invariant Cross-Section Ratios of Different Jet Radii for pp Full Jet Spectra 8 TeV with Comparison to PYTHIA8
|
|
| $\mathrm{D_{s2}^{*+}} /\mathrm{D_{s}^{+}} $ corrected-yield ratio vs multiplicity
|
|
| $\mathrm{D_{s1}^{+}} /\mathrm{D_{s}^{+}} $ corrected-yield ratio vs multiplicity
|
|
| $\mathrm{D_{s1}^{+}}$-, $\mathrm{D_{s2}^{*+}}$-, and $\mathrm{D_{s}^{+}}$-meson corrected yields vs multiplicity
|
|
| Invariant-mass distribution of $\mathrm{D_{s2}^{*+}}$ mesons in HM pp collisions at 13 TeV
|
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| Invariant-mass distribution of $\mathrm{D_{s2}^{*+}}$ mesons in MB pp collisions at 13 TeV
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