Public Preliminary figures by analysis
$\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
Invariant mass distribution of $\mathrm{D^-}\pi^+$pairs in the $1<\pt<23.5~\mathrm{GeV}/c$ interval in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
- Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
$\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
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)
- Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
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)
- Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
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)
- Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
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)
- Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
Ratio of the $R_{\rm T}$-dependent per-event D$^0$ meson yields to the $R_{\rm T}$-integrated yield in the toward region
- Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Acceptance-times-efficiency correction of D$^0$ mesons as a function of the $R_{\rm T}$
- Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Invariant mass distribution of D$^0$ candidates with 12 < $p_{\rm T}^{\rm D^0}$ < 18 GeV/$c$ in $R_{\rm T}$ > 1 events
- Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Invariant mass distribution of D$^0$ candidates with 5 < $p_{\rm T}^{\rm D^0}$ < 8 GeV/$c$ in $R_{\rm T}$ < 1 events
- Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
Inclusive charged-particle jet invariant yield in pp collisions at \sqrt{s} = 13.6 TeV
- Fig. Group : Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
- Fig. Group : Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Relative uncertainties of inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
- Fig. Group : Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
Ratio of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c with fit
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c with HT calculation
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c with model+nPDF bands
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EECs in p-Pb/pp for 60-80 GeV/c jets
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EECs in p-Pb/pp for 40-60 GeV/c jets
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EECs in p-Pb/pp for 20-40 GeV/c jets
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Fitted EEC peak heights in p-Pb
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Fitted EEC peak positions in p-Pb
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Fit of EECs for 60-80 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Fit of EECs for 40-60 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Fit of EECs for 20-40 GeV/c jets in p-Pb -- x (R_{L}) axis scaled by average jet pt
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EECs in p-Pb/pp for 60-80 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV)
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EECs in p-Pb/pp for 40-60 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV)
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 60-80 GeV/c jets
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 40-60 GeV/c jets
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
EEC distributions in p-Pb with varying track pT cut (150 MeV, 1 GeV, 2 GeV) for 20-40 GeV/c jets
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 60-80 GeV/c
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 40-60 GeV/c
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Comparison of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
EEC distributions of charged jets in p-Pb -- x (R_{L}) axis scaled by average jet pt
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EECs in p-Pb /pp for 20-40 GeV/c jets with CGC comparisons
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EECs in p-Pb/pp for 20-40 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV)
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Ratio of EECs in p-Pb and pp in different jet pT bins (20-40, 40-60, 60-80 GeV)
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
EEC distribution for charged jets in p-Pb collisions -- jet pT comparison (20-40, 40-60, 60-80 GeV)
- Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
p/pi in jets 3 curves
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
K/pi in jets 3 curves
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
pi spectra inclusive, jet+UE, UE
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
pi spectra inclusive and jet+UE
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
pi spectra inclusive only
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
p/pi in jets all 5 curves
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
K/pi in jets all 5 curves
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
p in jets spectra
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
K in jets spectra
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
pi in jets spectra - all four curves
- Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Substructure of charm-tagged jets in pp collisions at 13.6 TeV
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
nSD of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
nSD of D0-tagged jets in pp at 13.6 TeV
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Rg of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Rg of D0-tagged jets in pp at 13.6 TeV
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
$\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV compared with Run 2 results
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
zg of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
zg of D0-tagged jets in pp at 13.6 TeV
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
$\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV vs $\text{D}^{0}$
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
$\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV
- Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV with PYTHIA comparison
- Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV
- Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
R-ratio of R=0.2/R=0.4 recoil jets as a function of pT in 13.6 TeV, just Run 3 data
- Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Raw spectra of signal, reference and delta recoil vs pT for R=0.4 jets
- Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Delta recoil vs pT with PYTHIA comparison for R=0.4 jets in 13.6 TeV pp collisions
- Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Delta recoil vs pT with PYTHIA comparison for R=0.2 jets in 13.6 TeV pp collisions
- Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Delta recoil vs pT for R=0.4 jets in 13.6 TeV pp collisions
- Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Delta recoil vs pT for R=0.2 jets in 13.6 TeV pp collisions
- Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data
- PWG : PWG-JE (Jets)
- Energy: 13.6 TeV
- System: p-p
Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
Evolution of power index as a function of $\it{p}_{\rm{T}}$
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
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 $\it{p}_{\rm{T}}$
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
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
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
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 $\it{p}_{\rm{T}}$
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
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
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Empirical power law fit to normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
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 $\it{p}_{\rm{T}}$
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity with increasing upper limit of $\it{p}_{\rm{T}}$ windows
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Mean $\it{p}_{\rm{T}}$ as a function of charged particle multiplicity at fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Mean $\it{p}_{\rm{T}}$ as a function of charged particle multiplicity for increasing upper limit of $\it{p}_{\rm{T}}$ windows
- Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Jet substructure correlation of Soft Drop Rg and Zg
Ratio of zg distribution for wide and narrow jets in pp and Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
Ratio of θg distribution for balanced and unbalanced jets in pp and Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
zg distribution for wide jets in pp and Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
zg distribution for narrow jets in pp and Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
θg distribution for balanced jets in pp and Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
θg distribution for unbalanced jets in pp and Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb
zg distribution for wide jets in Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
zg distribution for narrow jets in Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
θg distribution for balanced jets in Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
θg distribution for unbalanced jets in Pb-Pb
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
zg distribution for wide jets in pp
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p
zg distribution for narrow jets in pp
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p
θg distribution for balanced jets in pp
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p
θg distribution for unbalanced jets in pp
- Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p
Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
Measurement spin alignment of prompt and non-prompt D∗+ mesons for both helicity and production frame in pp collisions at √s = 13.6 TeV
- Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Linear fit of #rho_{00}$ as function of non-promp fraction in both helicity and production frame
- Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
$\rho_{00}$ extraction in different cut of BDT score for non-prompt D* for helicity and production frame
- Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p
Measurement spin alignment of non-prompt D∗+ mesons compared to $J/\Psi$ meson measured by CMS
- Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13.6 TeV
- System: p-p