| Compilation of Invariant Cross-Sections for R = 0.3 in pp Full Jet Spectra - 5, 8, 13 TeV
|
|
| Compilation of Invariant Cross-Sections for R = 0.2 in pp Full Jet Spectra - 2.76, 5, 8, 13 TeV
|
|
| Compilation of Invariant Cross-Section Ratios of R = 0.2/0.5 in pp Full Jet Spectra - 5, 8, 13 TeV
|
|
| Compilation of Invariant Cross-Section Ratios of R = 0.2/0.4 in pp Full Jet Spectra - 2.76, 5, 8, 13 TeV
|
|
| Compilation of Invariant Cross-Section Ratios of R = 0.2/0.3 in pp Full Jet Spectra - 5, 8, 13 TeV
|
|
| Invariant Cross-Section Ratios of Different Jet Radii for pp Full Jet Spectra 8 TeV
|
|
| Invariant Cross-Section pp Full Jet Spectra 8 TeV, R = 0.2 -0.5
|
|
Fraction of Women in ALICE by Employment Category and Time (2014-2021, Final)
- PWG : Diversity Office
- Energy: none
- System none
|
|
| Fraction of events with trigger particle vs multiplicity
|
|
| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - Soft drop z_cut = 0.2, comparison with Hybrid model with Moliere scattering
|
|
| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - Dynamical grooming a = 2.0, comparison with Hybrid model with Moliere scattering
|
|
| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - Dynamical grooming a = 1.0, comparison with Hybrid model with Moliere scattering
|
|
| Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - Dynamical grooming a = 0.5, comparison with Hybrid model with Moliere scattering
|
|
| Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV compared with JETPHOX and NLO theory
|
|
| Direct photon spectra PbPb 5TeV ratios to model calculation, with PHENIX, 20-40%
|
|
| Charge conservation effect in first longitudinal coefficient a_{1} as a function of <dNch/deta> in Xe-Xe collisions
|
|
| $p_T$ dependence of $J/\psi$ $v_2$ for various collision systems
|
|
| Charge conservation effect in first longitudinal coefficient a_{1} as a function of <dNch/deta> in Pb-Pb collisions
|
|
| First longitudinal coefficient a_{1} scaled with sqrt(<dNch/deta>) as a function of <dNch/deta> in Pb-Pb and Xe-Xe collisions
|
|
| Direct photon spectra in PbPb 5.02TeV from PCM with comparison to all model calculations
|
|
| First longitudinal coefficient a_{1} in Xe-Xe and Pb-Pb collisions as a function of <dNch/deta>
|
|
| Direct photon double ratio in PbPb 5.02TeV from PCM with all models
|
|
| Procedure of $V_{2,J/\psi-tracklet}$ extraction from $V_{2,dimuon-tracklet}(m_{\mu\mu})$
|
|
| $p_T$ dependence of $J/\psi$ $v_2$ in pp collisions at 13 TeV - Yield subtraction method
|
|
| $p_T$ dependence of $J/\psi$ $v_2$ in pp collisions at 13 TeV
|
|
| Ratio of coherent $ J/\psi$ cross section measured in collisions with nuclear overlap over ultraperipheral Pb-Pb collisions at forward and midrapidity
|
|
| Coherent $ J/\psi$ cross section vs Npart in Pb-Pb collisions at $\sqrt{s_{\mathrm {NN}}}$ =5.02 TeV measured at midrapidty and forward rapidity
|
|
| Truncated mean of momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison
|
|
| Double ratio 0-20% from PCM and 0-10% from Dielectrons
|
|
| Double ratio 60-80% with different model calculations
|
|
| Double ratio 40-60% with different model calculations
|
|
| Double ratio 20-40% with different model calculations
|
|
| Double ratio 0-20% with different model calculations
|
|
| $\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Proton ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)
|
|
| $\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Kaon ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)
|
|
| $\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Pion ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)
|
|
| Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 5% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV
|
|
| Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 10% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| Isolated photons cross section comparison with theory and ratio
|
|
| 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 pp baseline
|
|
| Ratio of Lambda to K0s as a function of charge particle multiplicity
|
|
| 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 pp baseline
|
|
| 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 pp baseline
|
|
| Ratio of Lambda to K0s as a function of transverse momentum
|
|
| Purity: isolated photons purity distribution @ pp 8 TeV
|
|
| Ratio of Lambda yield to pions yield as a function of multiplicity
|
|
| 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 pp baseline
|
|
| Systematic Uncertainty: isolated photons cross section systematic uncertainties @ pp 8 TeV
|
|
| Ungroomed $\lambda_{\alpha=3}^{\kappa=1}$ 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 pp baseline
|
|
| Cross section: isolated photons cross section @ pp 8 TeV
|
|
| Ungroomed $\lambda_{\alpha=2}^{\kappa=1}$ 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 pp baseline
|
|
| Ungroomed $\lambda_{\alpha=1.5}^{\kappa=1}$ 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 pp baseline
|
|
| Cross section -- IsoGamma cross section in pp 13TeV
|
|
| Ratio of CS to theory comparison -- IsoGamma cross section in pp 13TeV
|
|
| CS and model pt comparison-- IsoGamma cross section in pp 13TeV
|
|
| CS comparison with theory -- pt and ratio -- IsoGamma cross section in pp 13TeV
|
|
| purity -- IsoGamma cross section in pp 13TeV
|
|
| Ratio of K0S yield to pions yield as a function of multiplicity
|
|
| SysUncertainty -- IsoGamma cross section in pp 13TeV
|
|
| Average transverse momentum as a function of multiplicity for Lambda including Pb-Pb data points
|
|
