| $\Omega^{-}$ DCA$_{z}$ fit with MC model in the interval 1.6 $\leq$ $p_{\mathrm{T}}$ < 2.0 GeV/c
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| $\Omega^{-}$ DCA$_{xy}$ fit with MC model in the interval 1.6 $\leq$ $p_{\mathrm{T}}$ < 2.0 GeV/c
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| Prompt $\Omega^{-}$ fraction as a function of $p_\mathrm{T}$
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [15;30] GeV/c
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [10;15] GeV/c
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [8;10] GeV/c
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [6;8] GeV/c
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [5;6] GeV/c
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [4;5] GeV/c
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [2;3] GeV/c
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [1;2] GeV/c
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| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [0;1] GeV/c
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| Comparison between of Ds+-h and D+h measurement away-side observables in differential pT bins of D meson and associated particles
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| Comparison between of Ds+-h and D+h measurement near-side observables in differential pT bins of D meson and associated particles
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| Comparison of near-side observables with PYTHIA 8 predictions in differential pT bins of Ds+ meson and associated particles
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| Comparison of away-side observables with PYTHIA 8 predictions in differential pT bins of Ds+ meson and associated particles
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| Baseline of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
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| Near-side width of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
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| Away-side width of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
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| Away-side yield of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
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| Near-side yield of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
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| Baseline comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Near-side yield comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Away-side yield comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Away-side widths comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Near-side widths comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Near-side yield comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Away-side yield comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Away-side width comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Near-side width comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)
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| Comparison between measured Ds-h and D+-h azimuthal correlation distributions (5 < $p_{T}$ < 8 GeV/c)
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| Comparison between measured Ds-h and D+-h azimuthal correlation distributions (3 < $p_{T}$ < 5 GeV/c)
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| Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (1 < $p_{T}$ < 3 GeV/c)
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| Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (3 < $p_{T}$ < 5 GeV/c)
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| Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (5 < $p_{T}$ < 8 GeV/c)
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| Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (8 < $p_{T}$ < 16 GeV/c)
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| Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (16 < $p_{T}$ < 36 GeV/c)
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| J/ψ σ/<v2> (including CMS comparison) vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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| J/ψ σ/<v2> vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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| J/ψ v24/v22 and σ/<v2> vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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| J/ψ v2{2}, v2{4}, v2{EP} and v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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| J/ψ v2{SP} and v2{4} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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| J/ψ v2{2} and v2{4} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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| J/ψ v2{2}, v2{EP} and v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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| J/ψ v2{2} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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| Non-prompt J/$\psi$~fraction in ALICE pp 13.6 TeV compared to ATLAS
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| 2-dimensional unbinned likelihood fit for fB (non-prompt J/$\psi$~fraction calculation)
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| Invariant mass distribution m_{ee} (non-prompt J/$\psi$~fraction calculation)
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| Background pseudoproper decay time distribution (non-prompt J/$\psi$~fraction calculation)
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| J/ψ v2{EP} vs centrality at forward rapidity in the dimuon channel for pt < 5 GeV/c and 5 < pT < 15 GeV/c at 5.36 TeV
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| Run 3 Non-prompt J/$\psi$~fraction in pp at 13.6 TeV compared to Run 2
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| J/ψ v2{SP} vs centrality at forward rapidity in the dimuon channel for pt < 5 GeV/c and 5 < pT < 20 GeV/c at 5.36 TeV
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| J/ψ v2 vs pT for the centrality class 30-50% and at 5.36 TeV compared to D0 and Upsilon(1S)
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| Non-prompt J/$\psi$ fraction in pp at 13.6 TeV (Run 3)
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| J/ψ v2{EP} vs pT at forward rapidity in the dimuon channel for the centrality classes 10-30%, 30-50%, 50-80% and at 5.36 TeV
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| J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality classes 0-10%, 10-30%, 30-50% and at 5.36 TeV
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| J/ψ v2{EP} vs pT at forward rapidity in the dimuon channel for the centrality class 30-50% and at 5.36 TeV (wider pT bins)
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| J/ψ v2{EP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV (wider pT bins)
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| J/ψ v2{EP} vs centrality at forward rapidity in the dimuon channel for 5 < pT < 15 GeV/c and at 5.36 TeV compared to Run 2
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| J/ψ v2{EP} vs centrality at forward rapidity in the dimuon channel for pT < 5 GeV/c and at 5.36 TeV compared to Run 2
|
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| J/ψ v2{SP} vs centrality at forward rapidity in the dimuon channel for 5 < pT < 20 GeV/c and at 5.36 TeV compared with Run 2
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| J/ψ v2{SP} vs centrality at forward rapidity in the dimuon channel for pT < 5 GeV/c and at 5.36 TeV compared to Run 2
|
|
| J/ψ v2{EP} vs pT at forward rapidity in the dimuon channel for the centrality class 30-50% and at 5.36 TeV compared to Run 2
|
|
| J/ψ v2{EP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV compared to Run 2
|
|
| J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 0-10% and at 5.36 TeV compared to Run 2
|
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| J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 30-50% and at 5.36 TeV compared to Run 2
|
|
| 2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [3;4] GeV/c
|
|
| J/ψ v2{EP} vs centrality at forward rapidity in the dimuon channel for 5 < pT < 15 GeV/c and at 5.36 TeV
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| J/ψ v2{EP} vs centrality at forward rapidity in the dimuon channel for pT < 5 GeV/c and at 5.36 TeV
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|
| J/ψ v2{EP} vs pT at forward rapidity in the dimuon channel for the centrality class 30-50% and at 5.36 TeV
|
|
| J/ψ v2{EP} vs pT at forward rapidity in the dimuon channel for the centrality class 30-50% and at 5.36 TeV
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|
| J/ψ v2{EP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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|
| J/ψ v2{SP} vs centrality at forward rapidity in the dimuon channel for 5 < pT < 20 GeV/c and at 5.36 TeV
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| J/ψ v2{SP} vs centrality at forward rapidity in the dimuon channel for pT < 5 GeV/c and at 5.36 TeV
|
|
| Prompt/non-prompt $J/\psi$ fraction at forward rapidity as a function of $p_{T}$
|
|
| J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 0-10% and at 5.36 TeV
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|
| J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 30-50% and at 5.36 TeV
|
|
| J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
|
|
| ϒ(1S) v2 calculation at fwd rapidity for the centality class 5-60%, pT class 0-3 GeV/c at 5.36 TeV, with the v2 background parametrized by the Chebyshev function
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| ϒ(1S) v2 calculation at fwd rapidity for the centality class 5-60%, pT class 0-3 GeV/c at 5.36 TeV, with the v2 background parametrized by Pol2
|
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| Cut variation of $\Lambda_c$ in pt 2 to 3 geV/c in pp collisions at 13.6 TeV
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| p-$\Lambda_c$ inv.mass in mixed-event in pp collisions at 13.6 TeV
|
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| p-$\Lambda_c$ inv.mass in same-event in pp collisions at 13.6 TeV
|
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| p-$\Lambda_c$ raw correlation function compare with models included strong interaction in pp collisions at 13.6 TeV
|
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| p-$\Lambda_c$ raw correlation function fit decomposition in pp collisions at 13.6 TeV
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| p-$\Lambda_c$ raw correlation function fit with coulomb only and background in pp collisions at 13.6 TeV
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| Ds1+/Ds ratio, (BR factorized)
|
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| Ds2*/Ds ratio, (BR factorized)
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| Ds2*/Ds ratio
|
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| Ds1+/Ds ratio
|
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| Ds, Ds1+ and Ds2* cross section
|
|
| Ds1+ Invariant Mass 2<pT<3 GeV/c
|
|
| Ds1+ Invariant Mass 6<pT<8 GeV/c
|
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| Ds1+ Invariant Mass 12<pT<24 GeV/c
|
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| Ds2* Invariant Mass 12<pT<24 GeV/c
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| Ds2* Invariant Mass 6<pT<8 GeV/c
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| Ds2* Invariant Mass 2<pT<4 GeV/c
|
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| Comparison between CMS and ALICE for the 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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| Comparison between the Blast wave description and Run 3 for the 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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| Comparison between models (TAMU and BBJS) and Run 3 for the 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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