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Public Preliminary figures by analysis

Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data

Raw spectra of signal, reference and delta recoil vs delta phi for R=0.4 jets in Pb-Pb collisions
Raw spectra of signal, reference and delta recoil vs delta r for R=0.4 jets in Pb-Pb collisions
Raw spectra of signal, reference and delta recoil vs delta r for R=0.4 jets in pp collisions
Raw spectra of signal, reference and delta recoil vs delta phi for R=0.4 jets in pp collisions

Measurement of the Lc cross section (integrated and vs multiplicity) in pp collisions at 13.6 TeV

Fit to the invariant-mass distribution of prompt $\Lambda_\text{c}$ in the $1<p_\text{T}<2\text{GeV}/c$ interval, multiplicity-integrated, in pp collisions at $\sqrt s = 13.6 \text{TeV}$
Fit to the invariant-mass distribution of prompt $\Lambda_\text{c}$ in the $8<p_\text{T}<10 \text{GeV}/c$ interval and $<\text{d}N_\text{ch}/\text{d}\eta> = 4.34$ in pp collisions at $\sqrt s = 13.6 \text{TeV}$
Fit to the invariant-mass distribution of prompt $\Lambda_\text{c}$ in the $4<p_\text{T}<5 \text{GeV}/c$ interval and $<\text{d}N_\text{ch}/\text{d}\eta> = 20.07$ in pp collisions at $\sqrt s = 13.6 \text{TeV}$
Ratio of $\Lambda_\text{c}$-to-$\text{D}^0$ cross section, pp collisions at $\sqrt s = 13.6 \text{TeV}$
Prompt $\Lambda_\text{c}$ cross section, pp collisions at $\sqrt s = 13.6 \text{TeV}$

Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity

J/ψ v2{2}, v2{4}, v2{EP}, v2{SP} and v2{SPRun2} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
J/ψ v2 vs pT for the centrality class 30-50% and at 5.36 TeV compared to prompt D0
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
J/ψ σ/<v2> vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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
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
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
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
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
J/ψ v2{2} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV
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
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
J/ψ v2 vs pT for the centrality class 30-50% and at 5.36 TeV compared to D0 and Upsilon(1S)
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
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
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)
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)
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
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
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
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
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
J/ψ v2{EP} vs centrality at forward rapidity in the dimuon channel for 5 < pT < 15 GeV/c and at 5.36 TeV
J/ψ v2{EP} vs centrality at forward rapidity in the dimuon channel for pT < 5 GeV/c 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
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 10-30% and at 5.36 TeV

$\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV

$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to forward-rapidity measurements by LHCb in $\mathrm{p-Pb}$ collisions and ALICE measurements in $\mathrm{Pb-Pb}$ collisions
Acceptance$\times$Efficiency correction for prompt $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons as a function of FT0M percentile and $\pt$ in pp collisions at $\sqrt{s}=13.6$ TeV
Fit to the raw-yield distribution of $\mathrm{D_s^+}$ mesons for different BDT non-prompt scores performed to extract the $\mathrm{D_s^+}$ $f_\mathrm{prompt}$ fraction with the cut-variation method
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $8< \pt <12$ GeV/$c$ interval and the $70-100\%$ FT0M percentile in pp collisions at $\sqrt{s}=13.6$ TeV
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $8< \pt <12$ GeV/$c$ interval and the $0-1\%$ FT0M percentile in pp collisions at $\sqrt{s}=13.6$ TeV
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <4$ GeV/$c$ interval and the $70-100\%$ FT0M percentile in pp collisions at $\sqrt{s}=13.6$ TeV
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <4$ GeV/$c$ interval and the $0-1\%$ FT0M percentile in pp collisions at $\sqrt{s}=13.6$ TeV

Y(1S) v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity

Y(1S) v2 vs pT for the centrality class 5-60% and at 5.36 TeV compared to non-prompt D0

J/ψ polarization at midrapidity in pp collisions at 13.6 TeV (QM2025)

Comparison with PbPb results in CS frame
Comparison with publiced results in pp collision in CS frame

Prompt and non-prompt J/$\psi$ separation at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV

Comparison of JPsi fB in mid and forward rapidities with other experiment results
Comparison of JPsi fB in mid and forward rapidities in pp at 13.6 TeV
Non-prompt J/$\psi$~fraction in ALICE pp 13.6 TeV compared to ATLAS
2-dimensional unbinned likelihood fit for fB (non-prompt J/$\psi$~fraction calculation)
Invariant mass distribution m_{ee} (non-prompt J/$\psi$~fraction calculation)
Background pseudoproper decay time distribution (non-prompt J/$\psi$~fraction calculation)
Run 3 Non-prompt J/$\psi$~fraction in pp at 13.6 TeV compared to Run 2
Non-prompt J/$\psi$ fraction in pp at 13.6 TeV (Run 3)

Measurement of the non-prompt $\Omega^{-}$ in pp collisions at $\sqrt{s}$ = 13.6 TeV

Comparison of the $\Omega^{-}$ baryons DCA_{z} distribution with and without the strangeness tracking
Comparison of the $\Omega^{-}$ baryons DCA_{xy} distribution with and without the strangeness tracking
DCA_{z} resolution of $\Omega^{-}$ baryons with and without the strangeness tracking
DCA_{xy} resolution of $\Omega^{-}$ baryons with and without the strangeness tracking
Invariant mass distribution of strangeness tracked $\Omega^{-}$ baryons
$\Omega^{-}$ DCA$_{z}$ fit with MC model in the interval 1.6 $\leq$ $p_{\mathrm{T}}$ < 2.0 GeV/c
$\Omega^{-}$ DCA$_{xy}$ fit with MC model in the interval 1.6 $\leq$ $p_{\mathrm{T}}$ < 2.0 GeV/c
Prompt $\Omega^{-}$ fraction as a function of $p_\mathrm{T}$

Prompt/non-prompt J/$\psi$ separation at foward rapidity in pp collisions at 13.6 TeV

2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [15;30] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [10;15] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [8;10] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [6;8] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [5;6] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [4;5] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [2;3] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [1;2] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [0;1] GeV/c
2D-fit between $J/\psi$ invariant mass and pseudo-proper decay length for pT range [3;4] GeV/c

$D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV

Comparison between of Ds+-h and D+h measurement away-side observables in differential pT bins of D meson and associated particles
Comparison between of Ds+-h and D+h measurement near-side observables in differential pT bins of D meson and associated particles
Comparison of near-side observables with PYTHIA 8 predictions in differential pT bins of Ds+ meson and associated particles
Comparison of away-side observables with PYTHIA 8 predictions in differential pT bins of Ds+ meson and associated particles
Baseline of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
Near-side width of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
Away-side width of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
Away-side yield of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
Near-side yield of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered
Baseline comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
Near-side yield comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
Away-side yield comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
Away-side widths comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
Near-side widths comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)
Near-side yield comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)
Away-side yield comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)
Away-side width comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)
Near-side width comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)
Comparison between measured Ds-h and D+-h azimuthal correlation distributions (5 < $p_{T}$ < 8 GeV/c)
Comparison between measured Ds-h and D+-h azimuthal correlation distributions (3 < $p_{T}$ < 5 GeV/c)
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (1 < $p_{T}$ < 3 GeV/c)
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (3 < $p_{T}$ < 5 GeV/c)
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (5 < $p_{T}$ < 8 GeV/c)
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (8 < $p_{T}$ < 16 GeV/c)
Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (16 < $p_{T}$ < 36 GeV/c)