Search for Preliminary Figures

Search for Preliminary Figures

Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 20% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV
Comparisons to models for KNO variables in the trans-min region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for KNO variables in the trans-max region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for KNO variables in the transverse region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for KNO variables in the trans-min region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for KNO variables in the trans-max region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for KNO variables in the transverse region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for KNO variables in the trans-min region in pp collisions at sqrt(s) = 2.76 TeV
Comparisons to models for KNO variables in the trans-max region in pp collisions at sqrt(s) = 2.76 TeV
Comparisons to models for KNO variables in the transverse region in pp collisions at sqrt(s) = 2.76 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-min region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-max region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for charged particles multiplicity distributions in the transverse region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-min region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-max region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for charged particles multiplicity distributions in the transverse region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-min region in pp collisions at sqrt(s) = 2.76 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-max region in pp collisions at sqrt(s) = 2.76 TeV
Comparisons to models for charged particles multiplicity distributions in the transverse region in pp collisions at sqrt(s) = 2.76 TeV
KNO variables in the trans-min region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 13 TeV
KNO variables in the trans-max region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 13 TeV
Charged particles multiplicity distributions in the trans-min region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 13 TeV
Charged particles multiplicity distributions in the trans-max region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 13 TeV
Charged particles multiplicity distributions in the transverse region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 13 TeV
Raw D0-Jet pT spectrum for D0 pT in the range 4 to 5 GeV/c
Invariant mass analysis (Kpi) in D0 pT range 10 to 12 GeV/c
Invariant mass analysis (Kpi) in D0 pT range 4 to 5 GeV/c
Results for $\phi$ meson production characterisation in pp collisions at $\sqrt{s}$ = 7 TeV
Prompt RAA vs pT for 0-50% Pb-Pb collisions at 5.02 TeV with Run 1 comparison
Non-prompt RAA vs pT for 0-50% Pb-Pb collisions at 5.02 TeV with Run 1 comparison
Prompt RAA vs pT for semicentral Pb-Pb collisions at 5.02 TeV with models
Non-prompt RAA vs pT for semicentral Pb-Pb collisions at 5.02 TeV with models
Prompt RAA vs pT for semicentral Pb-Pb collisions at 5.02 TeV
Non-prompt RAA vs pT for semicentral Pb-Pb collisions at 5.02 TeV
Prompt RAA vs pT for 10-30% Pb-Pb collisions at 5.02 TeV
Non-prompt RAA vs pT for 10-30% Pb-Pb collisions at 5.02 TeV
v2 in central p-Pb collisions with pi, K, p,Lambda using improved template fit method compared to AMPT with string melting
v2 in central p-Pb collisions with pi, K, p,Lambda using template fit method compared to AMPT with string melting
Ratio of eta meson invariant cross sections for 6 energies together with NLO calculations and Pythia
Ratio of pi0 invariant cross sections for 6 energies together with NLO calculations and Pythia
Prompt RAA vs pT for central Pb-Pb collisions at 5.02 TeV with models
Non-prompt RAA vs pT for central Pb-Pb collisions at 5.02 TeV with models
Prompt RAA vs pT for central Pb-Pb collisions at 5.02 TeV
Non-prompt RAA vs pT for central Pb-Pb collisions at 5.02 TeV
Prompt RAA vs Npart for Pb-Pb collisions at 5.02 TeV
Non-prompt RAA vs Npart for Pb-Pb collisions at 5.02 TeV
fB vs Npart for Pb-Pb collisions at 5.02 TeV with Run 1 comparison
fB vs pT central Pb-Pb collisions at 5.02 TeV with 0-50% Run 1 comparison
fb vs pT Pb-Pb collisions at 5.02 TeV with different centrality ranges and CMS comparison
fB vs pT 10-30% Pb-Pb collisions at 5.02 TeV with ATLAS comparison
fB vs pT semicentral Pb-Pb collisions at 5.02 TeV with ATLAS comparison
fB vs pT central Pb-Pb collision at 5.02 TeV with ATLAS comparison
Fb vs pT Pb-Pb collisions at 5.02 TeV with different centrality ranges
Likelihood fit projections in Pb-Pb central collisions at 5.02 TeV
simplified mee spectrum in 0-10% with POWHEG x Ncoll x RAA of HFe
simplified mee spectrum in 0-10% with POWHEG x Ncoll
Isolated photon cross section ratios in pp collisions $\sqrt s = $ 8 to 7 TeV
Isolated photon cross section ratios in pp collisions $\sqrt s = $ 13 to 8 TeV
Isolated photon cross section ratios in pp collisions $\sqrt s = $ 13 to 7 TeV
Acceptance Times Efficiency
Isolated photon cross section in pp collisions at $\sqrt s = $ 7, 8 and 13 TeV and p-Pb collisions at $\sqrt {s_{\rm NN}} = $ 5.02 TeV
Isolated photon cross section in pp collisions at $\sqrt s = $ 7, 8 and 13 TeV
Underlying event (UE) subtraction procedure for $z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 40-60 GeV/$c$ in p-Pb collisions at 5.02 TeV
Underlying event (UE) subtraction procedure for $\langle N_{\rm ch}\rangle$ distribution as a function of leading jet $p_{\rm T,jet}^{\rm ch}$ in p-Pb collisions at 5.02 TeV
Momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison
Angular correlations between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison
RAA and RpA for 1.1 < mee < 2.7 GeV/c2 as a function of pTee at 5 TeV
RAA and RpA for 0.5 < mee < 1.1 GeV/c2 as a function of pTee at 5 TeV
RAA and RpA as a function of mee at 5.02 TeV
DCAee spectrum in the IMR - templates scaled with fit result with Rapp
DCAee spectrum in the IMR - templates scaled with fit result
DCAee spectrum in the IMR -Ncoll cocktail scaled templates
DCAee spectrum in the IMR - HFe cocktail scaled templates with Rapp
DCAee spectrum in the IMR - HFe cocktail scaled templates
DCAee spectrum in the JPsi region - HFe cocktail scaled templates
DCAee spectrum in the JPsi region - Ncoll scaled templates
DCA template in the IMR - fit result
Ratio to JETPHOX of Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV
Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV
Raw 2d $\Delta_{recoil}$ distribution in pp collisions at $\sqrt{s} = 5.02$ TeV
Raw R=0.4 signal, reference and $\Delta_{recoil}$ recoil jet distribution in pp collisions at $\sqrt{\it{s}} = 5.02$ TeV
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
Isolated photons cross section ratio with theory prediction
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 pp baseline
Isolated photons cross section comparison with theory
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 pp baseline
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 pp baseline
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 pp baseline
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 pp baseline
Nuclear Modification Factor in p-Pb 8.16 TeV for K0S and Lambda