| Comparison between Run2 and Run 3 for the Y(1S) v2 as a function of centrality at fwd rapidity for the pT range 2-15 GeV/c
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| Y(1S) v2 as a function of centrality at fwd rapidity for the pT range 2-15 GeV/c at 5.36 TeV
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| Comparison between Run2 and Run 3 for the Y(1S) v2 as a function of pT at fwd rapidity for the centality class 5-60%
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| Y(1S) v2 as a function of pT at fwd rapidity for the centality class 5-60% at 5.36 TeV
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| Longitudinal polarization ($P_{\rm z}$) of prompt and non-prompt $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame)
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| Longitudinal polarization as a function of non-prompt fraction for $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame)
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| Simultaneous fit of $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ corrected yield as a function of $\cos(\theta^*)$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame)
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| Invariant mass distribution of ${\rm pK}\pi$ triplets in pp collisions at $\sqrt{s} = 13.6$ TeV in two intervals of $\cos(\theta^*)$ (production frame)
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| Ratio of the $R_{\rm T}$-dependent per-event D$^0$ meson yields to the $R_{\rm T}$-integrated yield in the toward region
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| Acceptance-times-efficiency correction of D$^0$ mesons as a function of the $R_{\rm T}$
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| Invariant mass distribution of D$^0$ candidates with 12 < $p_{\rm T}^{\rm D^0}$ < 18 GeV/$c$ in $R_{\rm T}$ > 1 events
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| Invariant mass distribution of D$^0$ candidates with 5 < $p_{\rm T}^{\rm D^0}$ < 8 GeV/$c$ in $R_{\rm T}$ < 1 events
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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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| 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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| p/pi in jets all 5 curves
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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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| pi in jets spectra - all four curves
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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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| 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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| 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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| Measurement spin alignment of prompt and non-prompt D∗+ mesons for both helicity and production frame in pp collisions at √s = 13.6 TeV
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| Linear fit of #rho_{00}$ as function of non-promp fraction in both helicity and production frame
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| $\rho_{00}$ extraction in different cut of BDT score for non-prompt D* for helicity and production frame
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| Measurement spin alignment of non-prompt D∗+ mesons compared to $J/\Psi$ meson measured by CMS
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| D* mesons raw yield extraction in the 10<pT<20 GeV/c interval in pp collisions at s√=13.6 TeV
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| Measurement spin alignment of prompt and non-prompt D∗+ mesons at production frame in pp collisions at √s = 13.6 TeV
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| Measurement spin alignment of prompt and non-prompt D∗+ mesons at helicity frame in pp collisions at √s = 13.6 TeV
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| Fit to the dimuon mass and v2 distribution for 5 < pT < 6 GeV at fwd rapidity for the centality class 10-50% and at 5.36 TeV
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| Fit to the dimuon mass and v2 distributions for 2 < pT < 3 GeV at fwd rapidity in Pb-Pb
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| Fit to the dimuon mass and v2 distributions for 0 < pT < 1 GeV at fwd rapidity in Pb-Pb
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| Fit to the dimuon mass and v2 distributions for 5 < pT < 6 GeV at fwd rapidity in Pb-Pb with event mixing background
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| Fit to the dimuon mass and v2 distributions for 0 < pT < 1 GeV at fwd rapidity in Pb-Pb with event mixing background
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| Fit to the dimuon mass and v2 distributions for 2 < pT < 3 GeV at fwd rapidity in Pb-Pb with event mixing background
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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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| ICP as a function of <Npart> for pT = 3-4 GeV/c in Pb-Pb collisions at 5.36 TeV
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| Invariant-mass distribution of $\mathrm{D^0}$ candidates with $12 < p_\mathrm{T} < 16$ in pp collisions at $\sqrt{s} = 13.6$ TeV
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| $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to PYTHIA 8, Catania and POWLANG predictions
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| $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at midrapidity $(\lvert y\rvert<0.5)$ at $\sqrt{s}=13.6$ TeV compared to forward-rapidity measurements by LHCb
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| $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to measurements by ALICE at different centre-of-mass energies
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| Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $5< \pt <5.5$ GeV/$c$ interval in pp collisions at $\sqrt{s}=13.6$ TeV
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| Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <2.5$ GeV/$c$ interval in pp collisions at $\sqrt{s}=13.6$ TeV
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