Public Preliminary figures by analysis
Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026]
Non-prompt $\psi$(2S) and J/$\psi$ fraction compare with EPOS4
- Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Non-prompt $\psi$(2S) fraction compare with EPOS4
- Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Non-prompt $\psi$(2S) fraction compare with measurements from other LHC experiments
- Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Non-prompt $\psi$(2S) fraction compare with non-prompt J/$\psi$ fraction
- Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Non-prompt $\psi$(2S) fraction in pp at 13.6 TeV
- Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
$D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
Ds-$\pi$ ULS-LS azimuthal correlation distribution (1 < $p_{T}$ < 3 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-$\pi$ ULS-LS azimuthal correlation distribution (3 < $p_{T}$ < 5 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-$\pi$ ULS-LS azimuthal correlation distribution (5 < $p_{T}$ < 8 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-$\pi$ ULS-LS azimuthal correlation distribution (8 < $p_{T}$ < 16 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-K ULS-LS azimuthal correlation distribution (8 < $p_{T}$ < 16 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-K ULS-LS azimuthal correlation distribution (5 < $p_{T}$ < 8 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-K ULS-LS azimuthal correlation distribution (3 < $p_{T}$ < 5 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-K ULS-LS azimuthal correlation distribution (1 < $p_{T}$ < 3 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (1 < $p_{T}$ < 3 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (3 < $p_{T}$ < 5 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (5 < $p_{T}$ < 8 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (8 < $p_{T}$ < 16 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-K ULS and LS azimuthal correlation distribution comparison (8 < $p_{T}$ < 16 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-K ULS and LS azimuthal correlation distribution comparison (5 < $p_{T}$ < 8 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-K ULS and LS azimuthal correlation distribution comparison (3 < $p_{T}$ < 5 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Ds-K ULS and LS azimuthal correlation distribution comparison (1 < $p_{T}$ < 3 GeV/c)
- Fig. Group : $D^{+}_{s}$-identified particles azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
[PWG-DQ] Hard Probes 2026 : Preliminary and performance figures
Comparison of polarization parameters with ICEM and CGC+NRQCD model predictions
- Fig. Group : [PWG-DQ] Hard Probes 2026 : Preliminary and performance figures
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Comparison of polarization parameters as a function of pT in pp 13.6 TeV with NRQCD model predictions
- Fig. Group : [PWG-DQ] Hard Probes 2026 : Preliminary and performance figures
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Comparison of polarization parameters as a function of pT in pp 13.6 TeV with 7 and 8 TeV
- Fig. Group : [PWG-DQ] Hard Probes 2026 : Preliminary and performance figures
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Polarization parameters as a function of pT in pp 13.6 TeV
- Fig. Group : [PWG-DQ] Hard Probes 2026 : Preliminary and performance figures
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
$D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV
Ds-meson invariant mass distribution (3 < $p_{T}$ < 5GeV/c)
- Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
Ds-h azimuthal correlation distribution (16 < $p_{T}$ < 36 GeV/c)
- Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
Ds-h azimuthal correlation distribution (8 < $p_{T}$ < 16 GeV/c)
- Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
Ds-h azimuthal correlation distribution (5 < $p_{T}$ < 8 GeV/c)
- Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
Ds-h azimuthal correlation distribution (3 < $p_{T}$ < 5 GeV/c)
- Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
Ds-h azimuthal correlation distribution (1 < $p_{T}$ < 3 GeV/c)
- Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
Ds-h ($\Delta\phi,\Delta\eta$) angular correlation distribution (8 < $p_{T}$ < 16 GeV/c)
- Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV, 5.36 TeV
- System: O-O, Pb-Pb
J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV, 5.36 TeV, 9.61 TeV
- System: O-O, p-O, Pb-Pb
J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV, 9.61 TeV
- System: O-O, p-O
J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV, 5.36 TeV, 8 TeV, 9.61 TeV
- System: O-O, p-O, Pb-Pb
J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: O-O
J/$\psi$ ROO vs pT in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: O-O
Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$
$\mathrm{\Lambda_{c}^{+}}/\mathrm{D}^0$ ratio in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$
- Fig. Group : Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Fit to the invariant-mass distribution of prompt $\mathrm{D}^{0}$ in the $3.5 < p_{\mathrm{T}} < 4 \mathrm{GeV}/c$ interval, in pp collisions at $\sqrt{s} = 13.6 \ \mathrm{TeV}$
- Fig. Group : Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ compared with FONLL
- Fig. Group : Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ compared with Run 2 measurement
- Fig. Group : Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Prompt and non-prompt J/$\psi$ separation at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV
fB in mid rapidities compared with PYTHIA comparisons
- Fig. Group : Prompt and non-prompt J/$\psi$ separation at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Inclusive J/psi production in midrapidity at 5.36TeV in pp collisions
The model comparison of differential cross section of inclusive J/psi at midrapidity in pp collisions at 5.36 TeV
- Fig. Group : Inclusive J/psi production in midrapidity at 5.36TeV in pp collisions
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: p-p
Differential cross section of inclusive J/psi at midrapidity in pp collisions at 5.36 TeV
- Fig. Group : Inclusive J/psi production in midrapidity at 5.36TeV in pp collisions
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: p-p
Preliminary measurement of prompt D-meson elliptic flow in OO collisions
Prompt $D^0$ elliptic flow comparison from semicentral Pb--Pb to central OO collisions
- Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O, Pb-Pb
Prompt $D^0$ elliptic flow comparison with light flavour hadrons
- Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
Charm meson elliptic flow in central OO collisions
- Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
$D^0$ meson simultaneous fit
- Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
$D^+$ meson simultaneous fit
- Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
$D_s^+$ meson simultaneous fit
- Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: O-O
J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026]
J/ψ v2 as a function of centrality at high pT in OO collisions, compared with results in Pb-Pb collisions
- Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: O-O
J/ψ v2 as a function of centrality at low pT in OO collisions, compared with results in Pb-Pb collisions
- Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: O-O
J/ψ v2 as a function of pT in semi-central OO collisions, compared with results in p-Pb and Pb-Pb collisions
- Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: O-O
J/ψ v2 as a function of pT in central OO collisions, compared with results in p-Pb and Pb-Pb collisions
- Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: O-O
J/ψ v2 as a function of pT in semi-central OO collisions compared with model calculations
- Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: O-O
J/ψ v2 as a function of pT in central OO collisions compared with model calculations
- Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.36 TeV
- System: O-O
J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV
Nuclear modification factor of J/psi in pO collisions as a function of pT, compared with p-Pb data and with FCEL model
- Fig. Group : J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 9.61 TeV
- System: p-O
Nuclear modification factor of J/psi in pO collisions as a function of pT, compared with p-Pb data
- Fig. Group : J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 9.61 TeV
- System: p-O
Nuclear modification factor of J/psi in pO collisions as a function of pT, compared with FCEL model
- Fig. Group : J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 9.61 TeV
- System: p-O
Nuclear modification factor of J/psi in pO collisions as a function of pT
- Fig. Group : J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 9.61 TeV
- System: p-O
D+-p femto in pp collisions at 13.6 TeV
Fit to the raw-yield distribution of $D^{+}$ mesons for different BDT non-prompt scores performed to extract the $D^{+}$ $f_{\mathrm{non-prompt}}$ fraction in the 1<pT<2 GeV/c in pp collisions at 13.6 TeV
- Fig. Group : D+-p femto in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Comparison of p$D^{-}$ momentum correlation function with model predictions in proton–proton collisions at 13.6 TeV
- Fig. Group : D+-p femto in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Comparison of p$D^{+}$ momentum correlation function with model predictions in proton–proton collisions at 13.6 TeV
- Fig. Group : D+-p femto in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Raw correlation function of p$D^{\pm}$ and simulation of non-femtosocpy background of p$D^{\pm}$ in proton–proton collisions at 13.6 TeV
- Fig. Group : D+-p femto in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Fit to the invariant-mass distribution of $D^{+}$ mesons in mixed events in the 0.06 < $k^{*}$ <0.10 GeV/c in proton–proton collisions at 13.6 TeV
- Fig. Group : D+-p femto in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Fit to the invariant-mass distribution of $D^{+}$ mesons in same events in the 0.06 < $k^{*}$ <0.10 GeV/c in proton–proton collisions at 13.6 TeV
- Fig. Group : D+-p femto in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Multiplicity dependence of prompt and non-prompt \jpsi~at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026]
Highest and lowest multiplicity nonprompt \jpsi~fB at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026]
- Fig. Group : Multiplicity dependence of prompt and non-prompt \jpsi~at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
Multiplicity dependence fB of \jpsi~at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026]
- Fig. Group : Multiplicity dependence of prompt and non-prompt \jpsi~at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026]
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
$\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV
$\Xi_c^+/\Lambda_c^+$ ratio compared with $\Xi_c^0/\Lambda_c^+$ by ALICE and $\Xi_c^+/\Lambda_c^+$ by LHCb
- Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with LHCb results
- Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with Run 2 results including $\Xi_c^+\rightarrow \Xi^- \pi^+ \pi^+$ and model predictions
- Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with Run 2 results and model predictions
- Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with Run 2 results
- Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
OmegaC production vs multiplicity in pp collisions at 13.6 TeV
BDT score for Omegac to Omega pi analysis in 4 < pT< 6 GeV/c in pp collisions at 13.6 TeV
- Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
ROC curve for Omegac to Omega pi analysis in 4 < pT< 6 GeV/c in pp collisions at 13.6 TeV
- Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
OmegaC self normalized yields in pp collisions at 13.6 TeV
- Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
OmegaC raw yield in 4_pT_6 and 10-50% FT0M
- Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
OmegaC raw yield in 4_pT_6 and 0-10% FT0M
- Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Measurement of charged B meson production in pp collisions in Run 3
B meson production cross section, comparison to kT factorization
- Fig. Group : Measurement of charged B meson production in pp collisions in Run 3
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
B meson production cross section, comparison phenomenological models, ratio
- Fig. Group : Measurement of charged B meson production in pp collisions in Run 3
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
B meson production cross section, comparison phenomenological models
- Fig. Group : Measurement of charged B meson production in pp collisions in Run 3
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
B meson production cross section, comparison FONLL, NNLO+NNL, ratio
- Fig. Group : Measurement of charged B meson production in pp collisions in Run 3
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
B meson production cross section, comparison FONLL, NNLO+NNL
- Fig. Group : Measurement of charged B meson production in pp collisions in Run 3
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
B meson production cross section, comparison to pQCD-based models, ratios
- Fig. Group : Measurement of charged B meson production in pp collisions in Run 3
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
B meson production cross section, comparison to pQCD-based models
- Fig. Group : Measurement of charged B meson production in pp collisions in Run 3
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p
B meson production cross section, comparison to data
- Fig. Group : Measurement of charged B meson production in pp collisions in Run 3
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13.6 TeV
- System: p-p, p-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
Ratio of $\pt$-integrated $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV to low-multiplicity pp collisions, compared to $\mathrm{K}^+/\pi^+$
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV, 13.6 TeV
- System: p-p, Pb-Pb
$\pt$-integrated $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV, compared to theoretical predictions
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV, 13.6 TeV
- System: p-p, Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV as a function of $\pt$
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV, 13.6 TeV
- System: p-p, Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV compared to PYTHIA 8 and EPOS4HQ predictions (EPOS4HQ highlight)
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV, 13.6 TeV
- System: p-p, Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV compared to PYTHIA 8 and EPOS4HQ predictions (PYTHIA highlight)
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV, 13.6 TeV
- System: p-p, Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV compared to PYTHIA 8 and EPOS4HQ predictions
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV, 13.6 TeV
- System: p-p, Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions compared at $\sqrt{s_\mathrm{NN}}=5.36$ TeV compared to LHCb measurement in p$-$Pb collisions
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV, 13.6 TeV
- System: p-p, Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV, 13.6 TeV
- System: p-p, Pb-Pb
Fit to the raw-yield distribution of $\mathrm{D^+}$ mesons for different BDT non-prompt scores performed to extract the $\mathrm{D^+}$ $f_\mathrm{prompt}$ fraction in the $2< \pt <4$ GeV/$c$ and $50-60\%$ FT0C interval
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: Pb-Pb
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 in the $2< \pt <4$ GeV/$c$ and $50-60\%$ FT0C interval
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: Pb-Pb
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <4$ GeV/$c$ interval and the $80-90\%$ FT0C percentile in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: Pb-Pb
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <4$ GeV/$c$ interval and the $0-10\%$ FT0C percentile in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 5.36 TeV
- System: Pb-Pb
Lambda longitudinal polarization in Run 3 OO collisions at 5.36 TeV
Longitudinal polarization Pz,s2 of Lambda + AntiLambda vs charged-particle multiplicity in OO and Pb-Pb collisions at 5.36 TeV
- Fig. Group : Lambda longitudinal polarization in Run 3 OO collisions at 5.36 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.36 TeV
- System: O-O, Pb-Pb