Search for Preliminary Figures

$\rho_{00}$ 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
$\rho_{00}$ 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
$\rho_{00}$ 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
Non-prompt fraction of $\mathrm{D}^{*+}$ candidates in 0-10% and 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
$|\cos{\vartheta^*}|$ 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
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
Direct photon pt (MB and HM)
$\rm D^{0}$-tagged raw jet axis distribution, $\Delta R_{\rm STD,D}$, for $R = 0.4$ in $10 < p_{\rm T,ch~ jet} < 20 {\rm ~ GeV}/c$
Fully corrected $\rm D^{0}$-tagged jet axis distribution, $\Delta R_{\rm STD,D}$, compared to PYTHIA 8 for $R = 0.4$ in $10 < p_{\rm T,ch~ jet} < 20 {\rm ~ GeV}/c$
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 $R=0.4$.
Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 30 - 50% Centrality and pp
Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp
Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 30 - 50% Centrality
Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10% Centrality
Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 30 - 50% Centrality
Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality
Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 30 - 50% Centrality
Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality
Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 30 - 50% Centrality and pp
Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 0 - 10% Centrality and pp
Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 30 - 50% Centrality and pp
Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 0 - 10% Centrality and pp
Comparison of $\lambda_{\theta}$ with UPC measurement
dNdcostheta vs costheta in Pb--Pb collisions at 5.02 TeV using Helicity Frame
Invariant mass distribution of dimuon pairs for 0.5 < |cos\theta| < 0.6 in Pb-Pb collsions at 5.02 TeV
Invariant mass distribution of dimuon pairs for 0.2 < |cos\theta| < 0.3 in Pb-Pb collsions at 5.02 TeV
Invariant mass distribution of dimuon pairs for 0.0 < |cos\theta| < 0.1 in Pb-Pb collsions at 5.02 TeV
Rg vs pt (HM)
Rg vs pt (MB)
Photon yield vs multiplicity (pp13TeV)
Direct photon pt (HM)
Direct photon pt (MB)
r vs pt HM (updated)
r vs pt MB (updated)
y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to ICEM+FONLL
pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to ICEM+FONLL
Integrated Upsilon(1S) and Upsilon(2S) cross section as a function of energy compared to ICEM+FONLL model calculations
pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to LHCb
y-differential upsilon(1S) pp cross section at 13 TeV compared to lower energy ALICE data
y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to LHCb
y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV
pT differential Upsilon(1S) and Upsilon(2S) cross section in pp collisions at 13 TeV
pT differential Upsilon(1S) cross section in pp collisions at 13 TeV compared to lower energy ALICE data
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - soft drop zcut = 0.2, comparison with models
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - soft drop zcut = 0.4, comparison with models
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - soft drop zcut = 0.2, comparison with models
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
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - Dynamical grooming a = 1.0, comparison with models
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - additional grooming methods comparison with PYTHIA8
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - selection of grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - additional grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - selection of grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - additional grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - original grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - selection of grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - additional grooming methods
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.
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.
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.
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.
EEC distribution for 40-60GeV charged jets in pp collision (theory comparison included)
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, $\alpha=1$.
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.
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.
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.
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.
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.
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
Away-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
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
Near-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
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
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
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
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
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.
$p_{\rm T}$-integrated non-prompt $\rm D^{0}$ $R_{\rm pPb}$ from 0-24 GeV/$\it{c}$ in pPb collisions at 5.02 TeV
Invariant-mass distribution of non-prompt $\rm D^{0}$ in pPb collisions at 5.02 TeV
Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV compared with CMS measurement in log scale
Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV compared with CMS measurement
$p_{\rm T}$-integrated non-prompt $\rm D^{0}$ $R_{\rm pPb}$ from 2-24 GeV/$\it{c}$ in pPb collisions at 5.02 TeV
Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV
Non-prompt $\rm D^{0}$ fractions