Search for Preliminary Figures

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
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
LcOverD0_pPb_pp
LcOverD0_pPb_PbPb
LcOverD0_pPb_3mult
LcOverD0_pPb_2mult
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
Acceptance Corrected 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 %
Mixed Event Acceptance Correction for In-Plane ch. + ne. jets, pT^jet = 20-40 GeV, pT^assoc. = 2-3 GeV, 5.02 TeV PbPb, 30-50 %
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 %
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 %
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 %
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 %
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 %
Mid/In Away Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Mid/In Near Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Out/In Away Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Out/In Near Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Away Side Constituent Yields, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Near Side Constituent Yields, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
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
$z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 40-60 GeV/$c$ in p-Pb collisions at 5.02 TeV
$z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 20-30 GeV/$c$ in p-Pb collisions at 5.02 TeV
$\langle N_{\rm ch}\rangle$ distribution as a function of leading jet $p_{\rm T,jet}^{\rm ch}$ in p-Pb collisions at 5.02 TeV
$\Upsilon$(1S) polarization as a function of transverse momentum
$\Upsilon$(1S) polarization: simultaneous fit to the corrected angular spectra in Helicity and Collins-Soper frames
$\Upsilon$(1S) polarization: Signal extraction
Direct photon double ratio in PbPb 5.02TeV from PCM with models
Direct photon double ratio in PbPb 5.02TeV from PCM with pQCD
Direct photon double ratio in PbPb 5.02TeV from PCM
Direct photon spectra PbPb 5TeV ratios to model calculation, LHC
Direct photon spectra PbPb 5TeV ratios to model calculation, with those from dielectrons and RHIC
Direct photon spectra ratios to model calculation
Direct photon spectra in PbPb 5.02TeV from PCM with comparison to pQCD
Lambda invariant for PbPb collisions at 5 TeV
Gamma-Gamma correlations in 30-50% PbPb collisions at 5 TeV, 0.35<kT<0.5 GeV/c
Gamma-Gamma correlations in 30-50% PbPb collisions at 5 TeV, 0.25<kT<0.35 GeV/c
Gamma-Gamma correlations in 0-10% PbPb collisions at 5 TeV, 0.35<kT<0.5 GeV/c
Gamma-Gamma correlations in 0-10% PbPb collisions at 5 TeV, 0.25<kT<0.35 GeV/c
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.5<kT<1.0 GeV/c
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.35<kT<0.5 GeV/c
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.25<kT<0.35 GeV/c
Direct photon double ratio in PbPb 5.02TeV from PCM and Dielectrons with comparison to model calculations
Direct photon spectra in PbPb 5.02TeV from PCM with comparison to model calculations
Direct photon spectra in PbPb 5.02TeV from PCM and Dielectrons with comparison to model calculations
Direct photon spectra in PbPb 5.02TeV from PCM
Omega Ratio Of Individual Measurements To Combined Fit in pp 13TeV
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
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
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
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
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
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
Lambda(1520)/Lambda yield ratio as a function of charged particle multiplicity
The strongly intensive quantity Σ in Pb-Pb and Xe-Xe collsions as a function of centrality
Example of template fit using four templates in 6 < pT < 8 GeV/c
Example of template fit using four templates in 1.3 < pT < 1.5 GeV/c
Ratio of beauty decay electrons in pp collisions at 13 TeV with one in pp collisions at 5.02 TeV
Ratio of beauty decay electrons in pp collisions at 13 TeV with ones in pp at 2.76, 5.02, and 7 TeV
Ratio of beauty decay electrons to heavy-flavour decay electrons in pp collisions at 13 TeV
Cross section of beauty decay electrons in pp collisions at 13 TeV
Corrected transverse momentum spectra of Lambda(1520) at 13 TeV
Lambda(1520) mean transverse momentum at \sqrt{s} = 5.02 and 13 TeV
Lambda(1520) pT integrated yield (dN/dy) at \srqt{s} = 5.02 TeV and 13 TeV
Corrected transverse momentum spectra of Lambda(1520) at 5.02TeV
$R$ and $\mu$ vs $k_{\mathrm T}$
$R$ and $\mu$ vs $<{\mathrm d}{N_{\mathrm {ch}}}/{\mathrm d}\eta>^{1/3}$
Correlation functions for pion-kaon pairs with their fits for 20-30% centrality
Correlation functions for pion-kaon pairs with non-femtoscopic background for Pb$-$Pb collisions at $\sqrt{s_{\mathrm {NN}}}=5.02$ for 20$-$30% centrality
Effect of hadronic resonance decays: Δη dependence
Scaled nudyn[+,-] Vs dNch/deta
Comparison with lower energies
S_{3} in p-Pb and pp collisions
  • Fig. Group : Hypertriton in pPb and pp
  • PWG : PWG-LF (Light Flavour Spectra)
  • Energy: 5.02 TeV
  • ,
  • Energy: 13 TeV
  • System p-p ,
  • System p-Pb
Hypertriton/$\Lambda$ in p-Pb and p-p
  • Fig. Group : Hypertriton in pPb and pp
  • PWG : PWG-LF (Light Flavour Spectra)
  • Energy: 5.02 TeV
  • ,
  • Energy: 13 TeV
  • System p-p ,
  • System p-Pb
nudyn[+,-] dependence on Δη in different momentum ranges
Δη dependence of the nudyn[+,-]
nudyn[+,-] scaled by mean multiplicities of accepted particles
nudyn[+,-] scaled by dNchdeta
nudyn[+,-] Vs dNch/deta for various collision systems
Correlation between v2 and [pT] of charged tracks in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region -- pp only HM -- IPGlasma + pp models
Correlation between v2 and [pT] of charged tracks in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region -- pp only HM -- IPGlasma+AMPT
Correlation between v2 and [pT] of charged tracks in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region -- pp only HM
Correlation between v2, v3, and [pT] of charged tracks in Pb--Pb collisions at 5.02 TeV
v2 fluctuations in Pb--Pb and pp collisions at 5.02 and 13 TeV
Dynamic [pT] fluctuations in Pb--Pb and pp collisions at 5.02 and 13 TeV
Covariance of v2-[pT] in Pb--Pb and pp collisions at 5.02 and 13 TeV