The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3 < y < 3.25
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The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.75 < y < 3
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The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.5 < y < 2.75
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The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT, pT < 3 GeV/c, in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
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The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
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y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV compared with one set of models of different scenarios
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y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
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Eta/Pi0 ratio as function of z for different jet pT intervals
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Ratio of Pi0 z spectra (Fragmentation function) for data and PYTHIA to parameterization
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Eta/Pi0 ratio inside jets as function of pT for different jet pT intervals
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Ratio of fully corrected Eta pT spectra inside jets (data and PYTHIA) to parameterization
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Eta pT spectra in different jet pT intervals normalized per jet
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Ratio of fully corrected Pi0 pT spectra inside jets (data and PYTHIA) to parameterization
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Pi0 pT spectra in different jet pT intervals normalized per jet
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Ratio of Eta pT spectra in different jet pT intervals to a fit to the inclusive Eta spectrum
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Eta pT spectra in different jet pT intervals normalized per event
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Ratio of Pi0 pT spectra in different jet pT intervals to a fit to the inclusive Pi0 spectrum
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Pi0 pT spectra in different jet pT intervals normalized per event and the inclusive Pi0 spectrum
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Pi0 pT spectra in different jet pT intervals normalized per event
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Comparison of corrected Eta spectra inside jets from different reconstruction methods as function of z
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Comparison of corrected Pi0 spectra inside jets from different reconstruction methods as function of z
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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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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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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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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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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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Response matrix for R=0.3 jets in central Pb-Pb collisions at 5.02 TeV
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Corrected jet $p_{T,jet}$ distribution with $p_{T}^{lead} > 5$ GeV/c for central Pb-Pb collisions at 5.02 TeV
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Raw correlated inclusive jet $p_{T,jet}^{reco}$ distribution for central Pb-Pb collisions at 5.02 TeV
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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
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Raw inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME for central Pb-Pb collisions at 5.02 TeV
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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
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Invariant Cross-Section Ratios of Different Jet Radii for pp Full Jet Spectra 8 TeV with Comparison to PYTHIA8
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Fragmentation function of J/psi-tagged charged jets
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Fragmentation function of non-prompt J/psi-tagged charged jets
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Fragmentation function of prompt J/psi-tagged charged jets
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f_B signal extraction 0.7 < z < 0.8
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Inclusive jpsi signal extraction, 0.7 < z < 0.8
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Fiducial cross section of Z->ee at mirapidity in pp collisions at 13 TeV
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Invariant mass of Z->ee (ULS and LS pairs) at midrapidity in pp collisions at 13 TeV
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Invariant mass of Z->ee at midrapidity in pp collisions at 13 TeV
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The comparison of longitudinal momentum fraction of $\rm D_{s}^{+}$ and $\rm D^{0}$ -tagged jets in MB pp collisions at 13 TeV
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Longitudinal momentum fraction of $\rm D_{s}^{+}$-tagged jets in MB pp collisions at 13 TeV
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Relative statistical and systematic uncertainties by categories of $\rm D_{s}^{+}$-tagged jets longitudinal momentum fraction in MB pp collisions at 13 TeV
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Feed-down contribution of $\rm D_{s}^{+}$ jets from POWHEG+PYTHIA6+EvtGen in MB pp collisions at 13 TeV
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Invariant mass distribution of $\rm D_{s}^{+}$ candidates inside jets in MB pp collisions at 13 TeV
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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
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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
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Energy flow distributions overview Charged jets 60-80 GeV pp 13 TeV, All Rjet pairs
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Energy flow distributions overview Charged jets 40-60 GeV pp 13 TeV, All Rjet pairs
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Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.35 to R=0.4
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Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.35 to R=0.4
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Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.2 to R=0.25
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Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.2 to R=0.25
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Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.05 to R=0.1
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Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.05 to R=0.1
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Mean energy flow versus jet radius with model comparison Charged jets 60-80 GeV pp 13 TeV
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Mean energy flow versus jet radius with model comparison Charged jets 40-60 GeV pp 13 TeV
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Mean energy flow versus jet radius with jet pt dependence Charged jets pp 13 TeV
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Measured $j_\mathrm{T}$ distributions in high $z$ bin compared to PYTHIA8 Tune4C
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Measured $j_\mathrm{T}$ distributions in mid $z$ bin compared to PYTHIA8 Tune4C
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Measured $j_\mathrm{T}$ distributions in low $z$ bin compared to PYTHIA8 Tune4C
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Measured $j_\mathrm{T}$ distributions in inclusive $z$ bin compared to PYTHIA8 Tune4C
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Measured $j_\mathrm{T}$ distributions in high $z$ bin compared to Herwig
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Measured $j_\mathrm{T}$ distributions in mid $z$ bin compared to Herwig
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