Public Preliminary figures by analysis
Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
Raw Jet-Hadron Correlation for In-Plane ch. + ne. jets, pT^jet = 20-40 GeV, pT^assoc. = 2-3 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Mid/In Away Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Mid/In Near Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Out/In Away Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Out/In Near Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Mid/In Away Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Mid/In Near Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Out/In Away Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Out/In Near Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Away Side Constituent Yields, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Near Side Constituent Yields, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
- Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Charged-particle jet properties in p-Pb collisions at 5.02 TeV
Unfolded and UE subtracted $z^{\rm ch}$ distributions for different leading jet $p_{\rm T,jet}^{\rm ch}$ in p-Pb collisions at 5.02 TeV
- Fig. Group : Charged-particle jet properties in p-Pb collisions at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
$z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 40-60 GeV/$c$ in p-Pb collisions at 5.02 TeV
- Fig. Group : Charged-particle jet properties in p-Pb collisions at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
$z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 20-30 GeV/$c$ in p-Pb collisions at 5.02 TeV
- Fig. Group : Charged-particle jet properties in p-Pb collisions at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
$\langle N_{\rm ch}\rangle$ distribution as a function of leading jet $p_{\rm T,jet}^{\rm ch}$ in p-Pb collisions at 5.02 TeV
- Fig. Group : Charged-particle jet properties in p-Pb collisions at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
$\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)
$\Upsilon$(1S) polarization as a function of transverse momentum
- Fig. Group : $\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
$\Upsilon$(1S) polarization: simultaneous fit to the corrected angular spectra in Helicity and Collins-Soper frames
- Fig. Group : $\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
$\Upsilon$(1S) polarization: Signal extraction
- Fig. Group : $\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 13 TeV
- System: p-p
Dijet Invariant mass analysis
Dijet invariant mass spectrum for pp and p-Pb including R_{pA} at 5.02 TeV
- Fig. Group : Dijet Invariant mass analysis
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Dijet invariant mass background fluctuations for charged jets R=0.4 for p-Pb 5.02 TeV
- Fig. Group : Dijet Invariant mass analysis
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-Pb
Dijet invariant mass background fluctuations for charged jets R=0.4 for pp 5.02 TeV
- Fig. Group : Dijet Invariant mass analysis
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: p-p
Direct photon R_gamma in PbPb 5.02TeV
Direct photon double ratio in PbPb 5.02TeV from PCM with models
- Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon double ratio in PbPb 5.02TeV from PCM with pQCD
- Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon double ratio in PbPb 5.02TeV from PCM
- Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon double ratio in PbPb 5.02TeV from PCM and Dielectrons with comparison to model calculations
- Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon spectra in PbPb 5.02TeV
Direct photon spectra PbPb 5TeV ratios to model calculation, LHC
- Fig. Group : Direct photon spectra in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon spectra PbPb 5TeV ratios to model calculation, with those from dielectrons and RHIC
- Fig. Group : Direct photon spectra in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon spectra ratios to model calculation
- Fig. Group : Direct photon spectra in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon spectra in PbPb 5.02TeV from PCM with comparison to pQCD
- Fig. Group : Direct photon spectra in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon spectra in PbPb 5.02TeV from PCM with comparison to model calculations
- Fig. Group : Direct photon spectra in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon spectra in PbPb 5.02TeV from PCM and Dielectrons with comparison to model calculations
- Fig. Group : Direct photon spectra in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Direct photon spectra in PbPb 5.02TeV from PCM
- Fig. Group : Direct photon spectra in PbPb 5.02TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
[QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
Lambda invariant for PbPb collisions at 5 TeV
- Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Gamma-Gamma correlations in 30-50% PbPb collisions at 5 TeV, 0.35<kT<0.5 GeV/c
- Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Gamma-Gamma correlations in 30-50% PbPb collisions at 5 TeV, 0.25<kT<0.35 GeV/c
- Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Gamma-Gamma correlations in 0-10% PbPb collisions at 5 TeV, 0.35<kT<0.5 GeV/c
- Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Gamma-Gamma correlations in 0-10% PbPb collisions at 5 TeV, 0.25<kT<0.35 GeV/c
- Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: Pb-Pb
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.5<kT<1.0 GeV/c
- Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: p-p
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.35<kT<0.5 GeV/c
- Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: p-p
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.25<kT<0.35 GeV/c
- Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 5.02 TeV
- System: p-p
Pi0-hadron correlations in PbPb at 5.02 TeV
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio with model comparison (zoomed out)
- Fig. Group : Pi0-hadron correlations in PbPb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio with model comparison (zoomed out)
- Fig. Group : Pi0-hadron correlations in PbPb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio (zoomed out)
- Fig. Group : Pi0-hadron correlations in PbPb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio (zoomed out)
- Fig. Group : Pi0-hadron correlations in PbPb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio with model comparison
- Fig. Group : Pi0-hadron correlations in PbPb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio with model comparison
- Fig. Group : Pi0-hadron correlations in PbPb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio
- Fig. Group : Pi0-hadron correlations in PbPb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio
- Fig. Group : Pi0-hadron correlations in PbPb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron femtoscopic study of correlation functions in PbPb
Pion-deuteron radii compared to predictions, Pb-Pb \sqrt{sNN}=5.02 TeV, $m_{T}$ = 1.03
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron radii compared to predictions, Pb-Pb \sqrt{sNN}=5.02 TeV, $m_{T}$ = 0.84 GeV/c
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron radii, multiplicity dependence, Pb-Pb \sqrt{sNN}=5.02 TeV
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pions and deuterons $m_{T}$ scaling Pb-Pb \sqrt{sNN}=5.02 TeV
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 30-50%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 10-30%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 0-10%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 30-50%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 10-30%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 0-10%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 30-50%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 10-30%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 0-10%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 30-50%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 10-30%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 0-10%
- Fig. Group : Pion-deuteron femtoscopic study of correlation functions in PbPb
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
[QM2022] - omega meson production in pp collisions at 13 TeV
Omega Ratio Of Individual Measurements To Combined Fit in pp 13TeV
- Fig. Group : [QM2022] - omega meson production in pp collisions at 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- Energy: 13 TeV
- System: p-p
Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ
Ratio of the strongly intensive quantity Σ to MC HIJING in Xe-Xe collisions at √sNN = 5.44 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
- Fig. Group : Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.44 TeV
- System: Xe-Xe
Ratio of the strongly intensive quantity Σ to MC HIJING in Pb-Pb collisions at √sNN = 5.02 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
- Fig. Group : Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Ratio of the strongly intensive quantity Σ to MC HIJING in Pb-Pb collisions at √sNN = 2.76 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
- Fig. Group : Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 2.76 TeV
- System: Pb-Pb
The strongly intensive quantity Σ in Xe-Xe collisions at √sNN = 5.44 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
- Fig. Group : Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.44 TeV
- System: Xe-Xe
The strongly intensive quantity Σ in Pb-Pb collisions at √sNN = 5.02 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
- Fig. Group : Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
The strongly intensive quantity Σ in Pb-Pb collisions at √sNN = 2.76 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
- Fig. Group : Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 2.76 TeV
- System: Pb-Pb
The strongly intensive quantity Σ in Pb-Pb and Xe-Xe collsions as a function of centrality
- Fig. Group : Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 2.76 TeV, 5.02 TeV, 5.44 TeV
- System: Pb-Pb, Xe-Xe
Lambda(1520) in pp collisions at 5.02 and 13 TeV
Lambda(1520)/Lambda yield ratio as a function of charged particle multiplicity
- Fig. Group : Lambda(1520) in pp collisions at 5.02 and 13 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV, 13 TeV
- System: p-p
Corrected transverse momentum spectra of Lambda(1520) at 13 TeV
- Fig. Group : Lambda(1520) in pp collisions at 5.02 and 13 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
Lambda(1520) mean transverse momentum at \sqrt{s} = 5.02 and 13 TeV
- Fig. Group : Lambda(1520) in pp collisions at 5.02 and 13 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV, 13 TeV
- System: p-p
Lambda(1520) pT integrated yield (dN/dy) at \srqt{s} = 5.02 TeV and 13 TeV
- Fig. Group : Lambda(1520) in pp collisions at 5.02 and 13 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV, 13 TeV
- System: p-p
Corrected transverse momentum spectra of Lambda(1520) at 5.02TeV
- Fig. Group : Lambda(1520) in pp collisions at 5.02 and 13 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
Measurement of electrons from beauty-hadron decays in pp collisions at 13 TeV with TPC+TOF
Example of template fit using four templates in 6 < pT < 8 GeV/c
- Fig. Group : Measurement of electrons from beauty-hadron decays in pp collisions at 13 TeV with TPC+TOF
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Example of template fit using four templates in 1.3 < pT < 1.5 GeV/c
- Fig. Group : Measurement of electrons from beauty-hadron decays in pp collisions at 13 TeV with TPC+TOF
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Ratio of beauty decay electrons in pp collisions at 13 TeV with one in pp collisions at 5.02 TeV
- Fig. Group : Measurement of electrons from beauty-hadron decays in pp collisions at 13 TeV with TPC+TOF
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Ratio of beauty decay electrons in pp collisions at 13 TeV with ones in pp at 2.76, 5.02, and 7 TeV
- Fig. Group : Measurement of electrons from beauty-hadron decays in pp collisions at 13 TeV with TPC+TOF
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Ratio of beauty decay electrons to heavy-flavour decay electrons in pp collisions at 13 TeV
- Fig. Group : Measurement of electrons from beauty-hadron decays in pp collisions at 13 TeV with TPC+TOF
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Cross section of beauty decay electrons in pp collisions at 13 TeV
- Fig. Group : Measurement of electrons from beauty-hadron decays in pp collisions at 13 TeV with TPC+TOF
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Non-identical particle (pion-kaon) femtoscopy in Pb$-$Pb collisions at 5.02 TeV with ALICE
$R$ and $\mu$ vs $k_{\mathrm T}$
- Fig. Group : Non-identical particle (pion-kaon) femtoscopy in Pb$-$Pb collisions at 5.02 TeV with ALICE
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
$R$ and $\mu$ vs $<{\mathrm d}{N_{\mathrm {ch}}}/{\mathrm d}\eta>^{1/3}$
- Fig. Group : Non-identical particle (pion-kaon) femtoscopy in Pb$-$Pb collisions at 5.02 TeV with ALICE
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Correlation functions for pion-kaon pairs with their fits for 20-30% centrality
- Fig. Group : Non-identical particle (pion-kaon) femtoscopy in Pb$-$Pb collisions at 5.02 TeV with ALICE
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Correlation functions for pion-kaon pairs with non-femtoscopic background for Pb$-$Pb collisions at $\sqrt{s_{\mathrm {NN}}}=5.02$ for 20$-$30% centrality
- Fig. Group : Non-identical particle (pion-kaon) femtoscopy in Pb$-$Pb collisions at 5.02 TeV with ALICE
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)
K$^{*\pm}$/K$^0_{s}$ double ratio: high multiplicity K$^{*\pm}$/K$^0_{s}$ $p$\textsubscript{T} spectrum divided by the low multiplicity one
- Fig. Group : Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
K$^{*\pm}$ and K$^{*0}$ $p_{\rm T}$-integrated yields
- Fig. Group : Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
K$^{*\pm}$ and K$^{*0}$ mean $p_{\rm T}$ spectra
- Fig. Group : Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
K$^{*\pm}$ and K$^{*0}$ $p$\textsubscript{T} spectra
- Fig. Group : Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
K$^0_{s}\pi^{\pm}$ invariant mass distribution after the uncorrelated background subtraction
- Fig. Group : Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
K$^0_{s}$ $\pi^{\pm}$ invariant mass distribution
- Fig. Group : Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
Net-charge fluctuations nydyn[+,-] for various collision systems (EPS2021)
Effect of hadronic resonance decays: Δη dependence
- Fig. Group : Net-charge fluctuations nydyn[+,-] for various collision systems (EPS2021)
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Scaled nudyn[+,-] Vs dNch/deta
- Fig. Group : Net-charge fluctuations nydyn[+,-] for various collision systems (EPS2021)
- PWG : PWG-CF (Flow and Correlations)
- Energy: 2.76 TeV, 5.02 TeV, 5.44 TeV
- System: Pb-Pb, p-Pb, Xe-Xe
Comparison with lower energies
- Fig. Group : Net-charge fluctuations nydyn[+,-] for various collision systems (EPS2021)
- PWG : PWG-CF (Flow and Correlations)
- Energy: 2.76 TeV, 5.02 TeV, 5.44 TeV
- System: Pb-Pb, p-Pb, Xe-Xe
Hypertriton in pPb and pp
S_{3} in p-Pb and pp collisions
- Fig. Group : Hypertriton in pPb and pp
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV, 13 TeV
- System: p-p, p-Pb
Hypertriton/$\Lambda$ in p-Pb and p-p
- Fig. Group : Hypertriton in pPb and pp
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV, 13 TeV
- System: p-p, p-Pb
W production at midrapidity via single electrons in pp @ 13 TeV
Raw positrons from W candidates with isolation cuts in |y|<0.6 in pp collisions at 13 TeV
- Fig. Group : W production at midrapidity via single electrons in pp @ 13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p
Raw electrons from W candidates with isolation cuts in |y|<0.6 in pp collisions at 13 TeV
- Fig. Group : W production at midrapidity via single electrons in pp @ 13 TeV
- PWG : PWG-HF (Heavy Flavour)
- Energy: 13 TeV
- System: p-p