| 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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| 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 CGC comparisons
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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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| 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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| $\omega$/$\pi$ ratio of ALICE and PHENIX measurements
|
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| $\omega$/$\pi$ ratio for pp collisions at a center-of-mass energy of 5.02TeV.
|
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| $\omega$/$\pi$ ratio in pp collisions at a center-of-mass energy of 5.02 TeV in comparison to measurements and model calculations
|
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| Spectrum of \omega yield for inelastic pp collisions at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T}$
|
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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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| ppΛ correlation function in Run3
|
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| ppp correlation function in Run3
|
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| ppΛ correlation function in Run3 compared to Run 2
|
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| ppp correlation function in Run3 compared to Run 2
|
|
| $\Sigma_{\rm c}^{0,++}(2520)/\Sigma_{\rm c}^{0,++}(2455)$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV compared with PYTHIA 8 predictions with Mode2, with variations on parameter probQQ1toQQ0join_charm
|
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| $M({\rm pK\pi\pi}) - M({\rm pK\pi})$ distribution in the interval $8 < p_{\rm T} < 12$ GeV/$c$ in pp collisions at $\sqrt{s} = 13.6$ TeV
|
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| Invariant-mass fit of non-prompt $\rm D^0$ in pp collisions at 13.6 TeV
|
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| Non-prompt $\rm D^0$ fraction as a function of $p_{\rm T}$
|
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| Contributions of the estimated prompt and non-prompt $\rm D^0$ with the cut-variation method
|
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| Invariant-mass fit of non-prompt $\rm D^0$ in pp collisions at 13.6 TeV
|
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| Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Model comparisons
|
|
Omega over pion ratio as a function of the pion yield in pp collisions at 9 GeV, 7 TeV and 13.6 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 900 GeV
, - Energy: 7 TeV
, - Energy: 13.6 TeV
- System p-p
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|
Kaon over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 900 GeV
- System p-p
|
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| Proton over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data
|
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| EEC collision energy dependence
|
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| E3C/EEC ratio theory comparison for 60-80 GeV charged jets
|
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| E3C/EEC ratio theory comparison for 40-60 GeV charged jets
|
|
| E3C/EEC ratio theory comparison for 20-40 GeV charged jets
|
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| E3C/EEC ratio model comparison for 60-80 GeV charged jets
|
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| E3C/EEC ratio model comparison for 40-60 GeV charged jets
|
|
