| p/pi in jets 3 curves
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| K/pi in jets 3 curves
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| pi spectra inclusive, jet+UE, UE
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| pi spectra inclusive and jet+UE
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| pi spectra inclusive only
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| K/pi in jets all 5 curves
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| p in jets spectra
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| K in jets spectra
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| nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results
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| Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results
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| nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c
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| nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c
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| Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c
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| Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c
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| nSD of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results
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| nSD of D0-tagged jets in pp at 13.6 TeV
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| Rg of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results
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| Rg of D0-tagged jets in pp at 13.6 TeV
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| zg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results
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| $\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV compared with Run 2 results
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| zg of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c
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| zg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c
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| zg of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results
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| zg of D0-tagged jets in pp at 13.6 TeV
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| $\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV vs $\text{D}^{0}$
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| $\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV
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| Ratio of EECs in p-Pb/pp for 60-80 GeV/c jets
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| Ratio of EECs in p-Pb/pp for 40-60 GeV/c jets
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| Ratio of EECs in p-Pb/pp for 20-40 GeV/c jets
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| Fitted EEC peak heights in p-Pb
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| Fitted EEC peak positions in p-Pb
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| Fit of EECs for 60-80 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt
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| Fit of EECs for 40-60 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt
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| Fit of EECs for 20-40 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt
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| Ratio of EECs in p-Pb/pp for 60-80 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV)
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| Ratio of EECs in p-Pb/pp for 40-60 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV)
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| EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 60-80 GeV/c jets
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| EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 40-60 GeV/c jets
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| EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 20-40 GeV/c jets
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| Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 60-80 GeV/c
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| Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 40-60 GeV/c
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| Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c
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| R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV with PYTHIA comparison
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| R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV
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| R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV, just Run 3 data
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| Raw spectra of signal, reference and delta recoil vs pT for R=0.4 jets
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| Delta recoil vs pT with PYTHIA comparison for R=0.4 jets in 13.6 TeV pp collisions
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| Delta recoil vs pT with PYTHIA comparison for R=0.2 jets in 13.6 TeV pp collisions
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| Delta recoil vs pT for R=0.4 jets in 13.6 TeV pp collisions
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| Delta recoil vs pT for R=0.2 jets in 13.6 TeV pp collisions
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| Evolution of power index as a function of $\it{p}_{\rm{T}}$
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| Normalized $\it{p}_{\rm{T}}$ correlator as a function of mean $\it{p}_{\rm{T}}$ for fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$
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| Normalized $\it{p}_{\rm{T}}$ correlator as a function of mean $\it{p}_{\rm{T}}$ with increasing upper limit of $\it{p}_{\rm{T}}$ windows
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| Relative uncertainties of inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
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| Inclusive charged-particle jet invariant yield in pp collisions at \sqrt{s} = 13.6 TeV
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| Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
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| Comparison of Pythia8 (Monash) and EPOS models to normalized mean $\it{p}_{\rm{T}}$ correlator as charged particle multiplicity at fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$
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| Comparison of Pythia8 (Monash) and EPOS models to normalized mean $\it{p}_{\rm{T}}$ correlator as charged particle multiplicity for increasing upper limit of $\it{p}_{\rm{T}}$ windows
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| Empirical power law fit to normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity
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| Normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity for fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$
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| Normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity with increasing upper limit of $\it{p}_{\rm{T}}$ windows
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| Mean $\it{p}_{\rm{T}}$ as a function of charged particle multiplicity at fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$
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| Mean $\it{p}_{\rm{T}}$ as a function of charged particle multiplicity for increasing upper limit of $\it{p}_{\rm{T}}$ windows
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| Ratio of zg distribution for wide and narrow jets in pp and Pb-Pb
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| Ratio of θg distribution for balanced and unbalanced jets in pp and Pb-Pb
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| zg distribution for wide jets in pp and Pb-Pb
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| zg distribution for narrow jets in pp and Pb-Pb
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| θg distribution for balanced jets in pp and Pb-Pb
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| θg distribution for unbalanced jets in pp and Pb-Pb
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| zg distribution for wide jets in Pb-Pb
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| zg distribution for narrow jets in Pb-Pb
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| θg distribution for balanced jets in Pb-Pb
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| θg distribution for unbalanced jets in Pb-Pb
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| zg distribution for wide jets in pp
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| zg distribution for narrow jets in pp
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| θg distribution for balanced jets in pp
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| θg distribution for unbalanced jets in pp
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| EEC distributions of charged jets in p-Pb -- x (R_{L}) axis scaled by average jet pt
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|
| Ratio of EECs in p-Pb/pp for 20-40 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV)
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| Ratio of EECs in p-Pb and pp in different jet pT bins (20-40, 40-60, 60-80 GeV)
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| EEC distribution for charged jets in p-Pb collisions -- jet pT comparison (20-40, 40-60, 60-80 GeV)
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| $\rm D^{0}$-tagged jet axes difference distributions, $\Delta R_{\rm STD-SD}$ for varied SD $z_{\rm cut}$, with comparisons to MC in $10 < p_{\rm T, ch~jet} < 20~\rm{GeV}/c$ for $R=0.4$
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| $\rm D^{0}$-tagged jet axes difference distributions, $\Delta R_{\rm SD-D^{0}}$ and $\Delta R_{\rm WTA-SD}$ for SD $z_{\rm cut} = 0.2$, with comparisons to MC for $R=0.4$ in $10 < p_{\rm T, ch~jet} < 20~\rm{GeV}/c$
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| $\rm D^{0}$-tagged jet axes difference distributions, $\Delta R_{\rm SD-D^{0}}$ and $\Delta R_{\rm WTA-SD}$ for SD $z_{\rm cut} = 0.1$, with comparisons to MC for $R=0.4$ in $10 < p_{\rm T, ch~jet} < 20~\rm{GeV}/c$
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| D$^{0}$-tagged jet compared to inclusive jets EECs and to different MC models in 15 < $p_{\rm T, ch. jet}$ < 30 GeV/c for $R=0.4$.
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| D$^{0}$-tagged jet compared to inclusive jets EECs and to different MC models in 10 < $p_{\rm T, ch. jet}$ < 15 GeV/c for $R=0.4$.
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| D$^{0}$-tagged jet compared to inclusive jets EECs and to different MC models in 10 < $p_{\rm T, ch. jet}$ < 15 GeV/c and 15 < $p_{\rm T, ch. jet}$ < 30 GeV/c for $R=0.4$.
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| Feed-down fraction in D$^{0}$-tagged energy-energy correlator in 15 < $p_{\rm T, ch. jet}$ < 30 GeV/c and 5 < $p_{\rm T,D^{0}}$ < 30 GeV/c for R = 0.4.
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| D0-tagged jet compared to inclusive jet EECs in 10 < $p_{\rm T, ch. jet}$ < 15 GeV/c and 15 < $p_{\rm T, ch. jet}$ < 30 GeV/c for $R=0.4$.
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| D0-tagged jet compared to inclusive jet EECs in 15 < $p_{\rm T, ch. jet}$ < 30 GeV/c for $R=0.4$.
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| D0-tagged jet compared to inclusive jet EECs in 10 < $p_{\rm T, ch. jet}$ < 15 GeV/c for $R=0.4$.
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| $\rm D^{0}$-tagged jet axes difference distributions, $\Delta R_{\rm STD-D^{0}}$ and $\Delta R_{\rm STD-WTA}$, with comparisons to MC for $R=0.4$ in $10 < p_{\rm T, ch~jet} < 20~\rm{GeV}/c$
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| $\rm D^{0}$-tagged jet axes difference distributions, $\Delta R_{\rm SD-D^{0}}$ and $\Delta R_{\rm STD-SD}$, with variations of SD $z_{\rm cut}$ directly compared to MC for $R=0.4$ in $10 < p_{\rm T, ch~jet} < 20~\rm{GeV}/c$
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| $\rm D^{0}$-tagged jet axes difference distributions, $\Delta R_{\rm SD-D^{0}}$ and $\Delta R_{\rm STD-SD}$, with PYTHIA 8, HERWIG 7, SHERPA Lund, SHERPA Ahadic and variations of SD $z_{cut}$ in $10 < p_{\rm T, ch~jet} < 20~\rm{GeV}/c$ for $R=0.4$
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| Fully corrected $\rm D^{0}$-tagged jet axes difference distributions, $\Delta R_{\rm STD-D^{0}}$ and $\Delta R_{\rm WTA-D^{0}}$, with PYTHIA 8 for $R=0.4$ in $10 < p_{\rm T, ch~jet} < 20~\rm{GeV}/c$
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| J/ψ v2 vs pT at forward rapidity in the dimuon channel at 5.36 TeV vs J/ψ v2 at 5.02 TeV
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| J/ψ v2 vs pT at forward rapidity in the dimuon channel for the centrality class 10-50% and at 5.36 TeV
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| ICP as a function of <Npart> for pT = 4-6 GeV/c in Pb-Pb collisions at 5.36 TeV and comparison with Pb-Pb collisions at 2.76 TeV
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| ICP as a function of <Npart> for pT = 6-8 GeV/c in Pb-Pb collisions at 5.36 TeV
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| ICP as a function of <Npart> for pT = 4-6 GeV/c in Pb-Pb collisions at 5.36 TeV
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