| 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
|
|
| Dijet invariant mass background fluctuations for charged jets R=0.4 for p-Pb 5.02 TeV
|
|
| Dijet invariant mass background fluctuations for charged jets R=0.4 for pp 5.02 TeV
|
|
| 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
|
|
| 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)
|
|
| 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)
|
|
| Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio (zoomed out)
|
|
| Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio (zoomed out)
|
|
| 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
|
|
| Pion-deuteron radii compared to predictions, Pb-Pb \sqrt{sNN}=5.02 TeV, $m_{T}$ = 1.03
|
|
| Pion-deuteron radii compared to predictions, Pb-Pb \sqrt{sNN}=5.02 TeV, $m_{T}$ = 0.84 GeV/c
|
|
| Pion-deuteron radii, multiplicity dependence, Pb-Pb \sqrt{sNN}=5.02 TeV
|
|
| Pions and deuterons $m_{T}$ scaling Pb-Pb \sqrt{sNN}=5.02 TeV
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 30-50%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 10-30%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 0-10%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 30-50%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 10-30%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 0-10%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 30-50%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 10-30%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 0-10%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 30-50%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 10-30%
|
|
| Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 0-10%
|
|
| 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$-$30% centrality
|
|
| Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio with model comparison
|
|
| Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio with model comparison
|
|
| Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio
|
|
| Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio
|
|
| K$^{*\pm}$/K$^0_{s}$ double ratio: high multiplicity K$^{*\pm}$/K$^0_{s}$ $p$\textsubscript{T} spectrum divided by the low multiplicity one
|
|
| K$^{*\pm}$ and K$^{*0}$ $p_{\rm T}$-integrated yields
|
|
| K$^{*\pm}$ and K$^{*0}$ mean $p_{\rm T}$ spectra
|
|
| K$^{*\pm}$ and K$^{*0}$ $p$\textsubscript{T} spectra
|
|
| K$^0_{s}\pi^{\pm}$ invariant mass distribution after the uncorrelated background subtraction
|
|
| K$^0_{s}$ $\pi^{\pm}$ invariant mass distribution
|
|
| 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
|
|
| Raw positrons from W candidates with isolation cuts in |y|<0.6 in pp collisions at 13 TeV
|
|
| Raw electrons from W candidates with isolation cuts in |y|<0.6 in pp collisions at 13 TeV
|
|
| nudyn[+,-] dependence on Δη in different momentum ranges
|
|
| Δη dependence of the nudyn[+,-]
|
|
| nudyn[+,-] scaled by mean multiplicities of accepted particles
|
|
