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Public Preliminary figures by analysis

V0s in p-Pb 8.16 TeV

Average transverse momentum as a function of multiplicity for Lambda
Average transverse momentum as a function of multiplicity for K0s including Pb-Pb data points
Average transverse momentum as a function of multiplicity for K0s
pT integrated yield of Lambda as a function of multiplicity including Pb-Pb data points
pT integrated yield of Lambda as a function of multiplicity
pT integrated yield of K0s as a function of multiplicity including Pb-Pb data points
pT integrated yield of K0s as a function of multiplicity
Transverse momentum spectra of Anti-Lambda in p-Pb 8.16 TeV and ratio to NSD
Transverse momentum spectra of Anti-Lambda in p-Pb 8.16 TeV
Transverse momentum spectra of Lambda in p-Pb 8.16 TeV and ratio to NSD
Transverse momentum spectra of Lambda in p-Pb 8.16 TeV
Transverse momentum spectra of K^{0}_{S} in p-Pb 8.16 TeV and ratio to NSD
Transverse momentum spectra of K^{0}_{S} in p-Pb 8.16 TeV

Average D mesons production vs unweighted spherocity S0 in pp at $\sqrt{s}$ = 13 TeV

D-mesons self normalised yield vs spherocity in [20,81] $N_{\mathrm{trk}}$
D-mesons self normalised yield vs spherocity in [31,81] $N_{\mathrm{trk}}$
D-mesons self normalised yield vs spherocity in [20,30] $N_{\mathrm{trk}}$

Groomed and ungroomed jet angularities and mass in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV

Groomed $\lambda_{\alpha=3}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $100 < p_\text{T}^\text{ch jet} < 150$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=2}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $100 < p_\text{T}^\text{ch jet} < 150$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=1.5}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $100 < p_\text{T}^\text{ch jet} < 150$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $100 < p_\text{T}^\text{ch jet} < 150$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=3}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $100 < p_\text{T}^\text{ch jet} < 150$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=2}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $100 < p_\text{T}^\text{ch jet} < 150$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=1.5}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $100 < p_\text{T}^\text{ch jet} < 150$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $100 < p_\text{T}^\text{ch jet} < 150$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=3}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=2}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=1.5}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=3}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=2}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=1.5}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=3}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=2}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=1.5}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=3}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=2}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=1.5}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=3}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=2}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=1.5}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Groomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=3}^{\kappa=1}$ for $R=0.2$ jets in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=2}^{\kappa=1}$ for $R=0.2$ jets in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=1.5}^{\kappa=1}$ for $R=0.2$ jets in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models
Ungroomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Ungroomed $\lambda_{\alpha=1}^{\kappa=1}$ for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to models

Flow of identified particles in pp collisions with improved template fit

v2 of kaons in HM pp collisions template fit and improved template fit with ultra-long-range correlations
v2 of pions in HM pp collisions template fit and improved template fit with ultra-long-range correlations
v2 of protons in HM pp collisions template fit and improved template fit with ultra-long-range correlations
v2 in HM pp collisions with h, pi, K, p with improved template fit with base 20-100%
v2 in HM pp collisions with h, pi, K, p with improved template fit with base 50-100%

Reconstruction of Beauty Jets in Proton-Proton Collisions at sqrt{s}=13\,TeV

Template fit to untagged data sample for performance estimation
Template fit to b-tagged data sample for performance estimation
Purity for b-jet selection in 13 TeV pp
Efficiency for b-jet selection in 13 TeV pp
Comparison of b-jet fractions at 5.02 TeV and 13 TeV
Comparison of b-jet spectra at 5.02 and 13 TeV

Investigations of anisotropic flow using multiparticle azimuthal correlations

Symmetric cumulants SC(3,2) in pp with different 3-sub configurations
Multiplicity dependence of symmetric cumulants and normalized symmetric cumulants in pp collisions
Multiplicity dependence of nonlinear flow modes in pp and Pb--Pb collisions
Multiplicity dependence of vn{m} in pp collisions (larger multiplicity range)
Multiplicity dependence of vn{m} in pp collisions

Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions

Momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions
Angular correlations between isolated photons and jets in 5.02 TeV Pb-Pb collisions
Subtraction procedure with same/mixed event for momentum imbalance between isolated photons and jets in 0-30% Pb-Pb collisions
Subtraction procedure with total background for momentum imbalance between isolated photons and jets in 0-30% Pb-Pb collisions
Subtraction procedure with same/mixed event for angular correlations between isolated photons and jets in 0-30% Pb-Pb collisions
Subtraction procedure with total background for angular correlations between isolated photons and jets in 0-30% Pb-Pb collisions
Systematic uncertainties for momentum imbalance between isolated photons and jets in 50-90% Pb-Pb collisions
Systematic uncertainties for momentum imbalance between isolated photons and jets in 30-50% Pb-Pb collisions
Systematic uncertainties for momentum imbalance between isolated photons and jets in 0-30% Pb-Pb collisions
Systematic uncertainties for angular correlations between isolated photons and jets in 50-90% Pb-Pb collisions
Systematic uncertainties for angular correlations between isolated photons and jets in 30-50% Pb-Pb collisions
Systematic uncertainties for angular correlations between isolated photons and jets in 0-30% Pb-Pb collisions
Photon purity in 5.02 TeV Pb-Pb collisions

LcOverD0_pPb_5.02TeV

LcOverD0_pPb_pp
LcOverD0_pPb_PbPb
LcOverD0_pPb_3mult
LcOverD0_pPb_2mult

(Multi-)strange $\Lambda$ $\Xi$ and $\Omega$ production vs multiplicity and ZDC energy in pp at 13 TeV

Midrapidity multiplicity vs forward energy in double differential percentile classes (SPDcl-V0M)
$\Xi$ production vs midrapidity multiplicity and ZDC energy - fixed V0M classes
$\Omega$ production vs midrapidity multiplicity and ZDC energy - fixed SPDClusters classes
$\Lambda$ production vs midrapidity multiplicity and ZDC energy - fixed SPDClusters classes
$\Xi$ production vs midrapidity multiplicity and ZDC energy - fixed SPDClusters classes
$\Lambda$ $\Xi$ and $\Omega$ production vs midrapidity multiplicity and ZDC energy

D0-Jet in 0-10% Pb-Pb collisions at 5.02 TeV (2018)

D0-jet, inclusive charged-particle jets and D0 transverse momentum spectra steepness comparison
D0-Jet, inclusive charged-particle jets, and average D-mesons nuclear modification factor in 0-10% Pb-Pb collisions
D0-Jet and inclusive charged-particle jets nuclear modification factor in 0-10% Pb-Pb collisions
D0-Jet nuclear modification factor in 0-10% Pb-Pb collisions (Log x-axis)
D0-Jet nuclear modification factor in 0-10% Pb-Pb collisions (Linear x-axis)
D0-jet transverse momentum spectrum
D0-jet transverse momentum spectrum with scaled pp reference

W production at midrapidity via single electrons in pp @ 13 TeV

Multiplicity dependence of electrons from W boson and associate hadron production with W boson in pp collisions at 13 TeV with PYTHIA predictions
Multiplicity dependence of associate hadron production with W boson in pp collisions at 13 TeV with PYTHIA prediction
Multiplicity dependence of electrons from W boson and associate hadron production with W boson in pp collisions at 13 TeV
Multiplicity dependence of W boson production via electrons in pp collisions at 13 TeV with PYTHIA8 production
Multiplicity dependence of W boson production via electrons in pp collisions at 13 TeV