cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79128.v1/t19
title: "Figure 5d" of "Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Ratio Rout/Rside vs. mT for PI+- PI+- for centrality 0-5%
description: Measuring K$^0_{\rm S}$K$^0_{\rm S}$ and K$^{\rm \pm}$K$^{\rm \pm}$ 
three-dimensional femtoscopic correlations using Pb-Pb collisions at 
$\mathbf {\sqrt{s_{\rm NN}}=2.76}$ TeV

LHC ALICE collaboration
KchKch and K0sK0s femtoscopy from 2.76 TeV/nucleon Pb-Pb collision
0-10%, 10-30% and 30-50% centrality, -0.8 &lt; eta &lt; 0.8

We present the results of three-dimensional femtoscopic analyses for charged and neutral kaons recorded by ALICE in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. The $m_{\mathrm{T}}$ scaling predicted by pure hydrodynamic models appears to be broken in our data, which indicates the importance of the hadronic rescattering phase at LHC energies. A $k_{\mathrm{T}}$ scaling of pion and kaon source radii is observed instead. The time of maximal emission of the system is estimated using the three-dimensional femtoscopic analysis for kaons. The measured emission time is larger than that of pions. Our observations are well supported by the hydrokinetic model predictions. 
For correlation functions (Figure 2, Figure 3) the errors are statistical only, systematic uncertainties are equal to or less than the statistical errors.
For all other figures total errors are presented.
DOI: 10.17182/hepdata.79128.v1/t20
title: "Figure 7a" of "Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Ratio Rout/Rside vs. mT for PI+- PI+- for centrality 0-10%
description: Measuring K$^0_{\rm S}$K$^0_{\rm S}$ and K$^{\rm \pm}$K$^{\rm \pm}$ 
three-dimensional femtoscopic correlations using Pb-Pb collisions at 
$\mathbf {\sqrt{s_{\rm NN}}=2.76}$ TeV

LHC ALICE collaboration
KchKch and K0sK0s femtoscopy from 2.76 TeV/nucleon Pb-Pb collision
0-10%, 10-30% and 30-50% centrality, -0.8 &lt; eta &lt; 0.8

We present the results of three-dimensional femtoscopic analyses for charged and neutral kaons recorded by ALICE in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. The $m_{\mathrm{T}}$ scaling predicted by pure hydrodynamic models appears to be broken in our data, which indicates the importance of the hadronic rescattering phase at LHC energies. A $k_{\mathrm{T}}$ scaling of pion and kaon source radii is observed instead. The time of maximal emission of the system is estimated using the three-dimensional femtoscopic analysis for kaons. The measured emission time is larger than that of pions. Our observations are well supported by the hydrokinetic model predictions. 
For correlation functions (Figure 2, Figure 3) the errors are statistical only, systematic uncertainties are equal to or less than the statistical errors.
For all other figures total errors are presented.
DOI: 10.17182/hepdata.79128.v1/t21
title: "Figure 7b" of "Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Ratio Rout/Rside vs. mT for PI+- PI+- for centrality 10-30%
description: Measuring K$^0_{\rm S}$K$^0_{\rm S}$ and K$^{\rm \pm}$K$^{\rm \pm}$ 
three-dimensional femtoscopic correlations using Pb-Pb collisions at 
$\mathbf {\sqrt{s_{\rm NN}}=2.76}$ TeV

LHC ALICE collaboration
KchKch and K0sK0s femtoscopy from 2.76 TeV/nucleon Pb-Pb collision
0-10%, 10-30% and 30-50% centrality, -0.8 &lt; eta &lt; 0.8

We present the results of three-dimensional femtoscopic analyses for charged and neutral kaons recorded by ALICE in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. The $m_{\mathrm{T}}$ scaling predicted by pure hydrodynamic models appears to be broken in our data, which indicates the importance of the hadronic rescattering phase at LHC energies. A $k_{\mathrm{T}}$ scaling of pion and kaon source radii is observed instead. The time of maximal emission of the system is estimated using the three-dimensional femtoscopic analysis for kaons. The measured emission time is larger than that of pions. Our observations are well supported by the hydrokinetic model predictions. 
For correlation functions (Figure 2, Figure 3) the errors are statistical only, systematic uncertainties are equal to or less than the statistical errors.
For all other figures total errors are presented.
DOI: 10.17182/hepdata.79128.v1/t22
title: "Figure 7c" of "Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Ratio Rout/Rside vs. mT for PI+- PI+- for centrality 30-50%
description: Measuring K$^0_{\rm S}$K$^0_{\rm S}$ and K$^{\rm \pm}$K$^{\rm \pm}$ 
three-dimensional femtoscopic correlations using Pb-Pb collisions at 
$\mathbf {\sqrt{s_{\rm NN}}=2.76}$ TeV

LHC ALICE collaboration
KchKch and K0sK0s femtoscopy from 2.76 TeV/nucleon Pb-Pb collision
0-10%, 10-30% and 30-50% centrality, -0.8 &lt; eta &lt; 0.8

We present the results of three-dimensional femtoscopic analyses for charged and neutral kaons recorded by ALICE in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. The $m_{\mathrm{T}}$ scaling predicted by pure hydrodynamic models appears to be broken in our data, which indicates the importance of the hadronic rescattering phase at LHC energies. A $k_{\mathrm{T}}$ scaling of pion and kaon source radii is observed instead. The time of maximal emission of the system is estimated using the three-dimensional femtoscopic analysis for kaons. The measured emission time is larger than that of pions. Our observations are well supported by the hydrokinetic model predictions. 
For correlation functions (Figure 2, Figure 3) the errors are statistical only, systematic uncertainties are equal to or less than the statistical errors.
For all other figures total errors are presented.
DOI: 10.17182/hepdata.79128.v1/t23
title: "Figure 8" of "Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Rlong^2 vs. mT for PI+- PI+- for centrality 0-5%
description: Measuring K$^0_{\rm S}$K$^0_{\rm S}$ and K$^{\rm \pm}$K$^{\rm \pm}$ 
three-dimensional femtoscopic correlations using Pb-Pb collisions at 
$\mathbf {\sqrt{s_{\rm NN}}=2.76}$ TeV

LHC ALICE collaboration
KchKch and K0sK0s femtoscopy from 2.76 TeV/nucleon Pb-Pb collision
0-10%, 10-30% and 30-50% centrality, -0.8 &lt; eta &lt; 0.8

We present the results of three-dimensional femtoscopic analyses for charged and neutral kaons recorded by ALICE in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. The $m_{\mathrm{T}}$ scaling predicted by pure hydrodynamic models appears to be broken in our data, which indicates the importance of the hadronic rescattering phase at LHC energies. A $k_{\mathrm{T}}$ scaling of pion and kaon source radii is observed instead. The time of maximal emission of the system is estimated using the three-dimensional femtoscopic analysis for kaons. The measured emission time is larger than that of pions. Our observations are well supported by the hydrokinetic model predictions. 
For correlation functions (Figure 2, Figure 3) the errors are statistical only, systematic uncertainties are equal to or less than the statistical errors.
For all other figures total errors are presented.
DOI: 10.17182/hepdata.80519.v1/t5
title: "Table 5" of "First measurement of jet mass in Pb-Pb and p-Pb collisions at the LHC"

description: Jet mass distribution in PbPb collisions at cme 2760 GeV, pT,jet ch = 80-100 GeV/c
description: No data abstract available.
DOI: 10.17182/hepdata.80519.v1/t6
title: "Table 6" of "First measurement of jet mass in Pb-Pb and p-Pb collisions at the LHC"

description: Jet mass distribution in PbPb collisions at cme 2760 GeV, pT,jet ch = 100-120 GeV/c
description: No data abstract available.
DOI: 10.17182/hepdata.80519.v1/t7
title: "Table 7" of "First measurement of jet mass in Pb-Pb and p-Pb collisions at the LHC"

description: Mean of the jet mass distributions in pPb collisions as a function of pTjet ch
description: No data abstract available.
DOI: 10.17182/hepdata.80519.v1/t8
title: "Table 8" of "First measurement of jet mass in Pb-Pb and p-Pb collisions at the LHC"

description: Mean of the jet mass distributions in PbPb collisions as a function of pTjet ch
description: No data abstract available.
DOI: 10.5064/f6g2petf/0phsaw
title: Moore-et-al_MD_0221_Governor Larry Hogan - Official Website for the Governor of Maryland_25.pdf
DOI: 10.17182/hepdata.77359.v1/t1
title: "Table 1" of "W and Z boson production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Z-boson production cross section in the dimuon decay channel at backward and forward rapidities measured in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV. The first uncertainty is statistical, the second is systematic.
description: The W and Z boson production was measured via the muonic decay channel in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV at the Large Hadron Collider with the ALICE detector.
The measurement covers backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity regions, corresponding to Pb-going and p-going directions, respectively.
The Z-boson production cross section, with dimuon invariant mass of $6010$ GeV/$c$ are determined.
The W-boson production is also studied as a function of the collision centrality: the cross section of muons from W-boson decays is found to scale with the average number of binary nucleon-nucleon collisions within uncertainties.
DOI: 10.17182/hepdata.78365.v1/t4
title: "DN/DYRAP" of "Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Estimation of $\mathrm{d}N_{\mathrm{ch}}/\mathrm{d}y$ for in the most central Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$. Also shown is a fit of Gaussian distribution to the data.
description: CERN-LHC. We present the charged-particle pseudorapidity density in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$ in centrality classes measured by ALICE. The measurement covers a wide pseudorapidity range from $-3.5$ to $5$, which is sufficient for reliable estimates of the total number of charged particles produced in the collisions. For the most central collisions we find $21\,400\pm 1\,300$ while for the most peripheral we find $230\pm 38$. This corresponds to an increase of $(27\pm4)\%$ over the results at $\sqrt{s_{_{\mathrm{NN}}}}=2.76\,\mathrm{TeV}$ previously reported by ALICE. The energy dependence of the total number of charged particles produced in heavy-ion collisions is found to obey a modified power-law like behaviour. The charged-particle
pseudorapidity density of the most central collisions is compared to model calculations - none of which fully describes the measured distribution. We also present an estimate of the rapidity density of charged particles. The width of that distribution is found to exhibit a remarkable proportionality to the beam rapidity, independent of the collision energy from the top SPS to LHC energies.
DOI: 10.17182/hepdata.78365.v1/t5
title: "SIGMA DN/DYRAP" of "Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Scaling behaviour as a function $\sqrt{s_{_{\mathrm{NN}}}}$ of the width of the charged-particle or -pion rapidity-density distribution with respect to the Landau-Carruthers width (top) and rapidity range (bottom). Charged-pion points from AGS and SPS are adapted from the literature [PRL94.162301], while the PHOBOS (filled crosses) [PRL91,052303] and BRAHMS (open crosses) [PRL88.202301] charged-hadron points are translated from the corresponding $\mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ results.
description: CERN-LHC. We present the charged-particle pseudorapidity density in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$ in centrality classes measured by ALICE. The measurement covers a wide pseudorapidity range from $-3.5$ to $5$, which is sufficient for reliable estimates of the total number of charged particles produced in the collisions. For the most central collisions we find $21\,400\pm 1\,300$ while for the most peripheral we find $230\pm 38$. This corresponds to an increase of $(27\pm4)\%$ over the results at $\sqrt{s_{_{\mathrm{NN}}}}=2.76\,\mathrm{TeV}$ previously reported by ALICE. The energy dependence of the total number of charged particles produced in heavy-ion collisions is found to obey a modified power-law like behaviour. The charged-particle
pseudorapidity density of the most central collisions is compared to model calculations - none of which fully describes the measured distribution. We also present an estimate of the rapidity density of charged particles. The width of that distribution is found to exhibit a remarkable proportionality to the beam rapidity, independent of the collision energy from the top SPS to LHC energies.
DOI: 10.17182/hepdata.77359.v1/t2
title: "Table 2" of "W and Z boson production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Cross section of $\mu^{+}$ from W$^{+}$ boson decay at backward and forward rapidities measured in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV. The first uncertainty is statistical, the second is systematic.
description: The W and Z boson production was measured via the muonic decay channel in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV at the Large Hadron Collider with the ALICE detector.
The measurement covers backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity regions, corresponding to Pb-going and p-going directions, respectively.
The Z-boson production cross section, with dimuon invariant mass of $6010$ GeV/$c$ are determined.
The W-boson production is also studied as a function of the collision centrality: the cross section of muons from W-boson decays is found to scale with the average number of binary nucleon-nucleon collisions within uncertainties.
DOI: 10.17182/hepdata.77359.v1/t3
title: "Table 3" of "W and Z boson production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Cross section of $\mu^{-}$ from W$^{-}$ boson decay at backward and forward rapidities measured in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV. The first uncertainty is statistical, the second is systematic.
description: The W and Z boson production was measured via the muonic decay channel in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV at the Large Hadron Collider with the ALICE detector.
The measurement covers backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity regions, corresponding to Pb-going and p-going directions, respectively.
The Z-boson production cross section, with dimuon invariant mass of $6010$ GeV/$c$ are determined.
The W-boson production is also studied as a function of the collision centrality: the cross section of muons from W-boson decays is found to scale with the average number of binary nucleon-nucleon collisions within uncertainties.
DOI: 10.17182/hepdata.77359.v1/t4
title: "Table 4" of "W and Z boson production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Lepton charge asymmetry of muons from W-boson decays at backward and forward rapidities measured in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV. The first uncertainty is statistical, the second is systematic.
description: The W and Z boson production was measured via the muonic decay channel in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV at the Large Hadron Collider with the ALICE detector.
The measurement covers backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity regions, corresponding to Pb-going and p-going directions, respectively.
The Z-boson production cross section, with dimuon invariant mass of $6010$ GeV/$c$ are determined.
The W-boson production is also studied as a function of the collision centrality: the cross section of muons from W-boson decays is found to scale with the average number of binary nucleon-nucleon collisions within uncertainties.
DOI: 10.17182/hepdata.78365.v1/t1
title: "DN/DETARAP" of "Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Charged-particle pseudorapidity density for ten centrality classes over a broad $\eta$ range in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$. Boxes around the points reflect the total uncorrelated systematic uncertainties, while the filled squares on the right reflect the correlated systematic uncertainty (evaluated at $\eta=0$). Statistical errors are generally insignificant and smaller than the markers. Also shown is the reflection of the $3.5&lt;\eta&lt;5$ values around $\eta=0$ (open circles). The line corresponds to fits of the difference between two Gaussians centred at $\eta=0$ ($f_{\text{GG}}$) [PLB754.373] to the data.
description: CERN-LHC. We present the charged-particle pseudorapidity density in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$ in centrality classes measured by ALICE. The measurement covers a wide pseudorapidity range from $-3.5$ to $5$, which is sufficient for reliable estimates of the total number of charged particles produced in the collisions. For the most central collisions we find $21\,400\pm 1\,300$ while for the most peripheral we find $230\pm 38$. This corresponds to an increase of $(27\pm4)\%$ over the results at $\sqrt{s_{_{\mathrm{NN}}}}=2.76\,\mathrm{TeV}$ previously reported by ALICE. The energy dependence of the total number of charged particles produced in heavy-ion collisions is found to obey a modified power-law like behaviour. The charged-particle
pseudorapidity density of the most central collisions is compared to model calculations - none of which fully describes the measured distribution. We also present an estimate of the rapidity density of charged particles. The width of that distribution is found to exhibit a remarkable proportionality to the beam rapidity, independent of the collision energy from the top SPS to LHC energies.
DOI: 10.17182/hepdata.78365.v1/t2
title: "DN/DETARAP(ETARAP=0)" of "Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Charged-particle pseudorapidity density at midrapidity in most perihperhal (80-90%) Pb-Pb collisions at $\sqrt{s_{\scriptscriptstyle\mathrm{NN}}}=5.02\,\mathrm{TeV}$.
description: CERN-LHC. We present the charged-particle pseudorapidity density in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$ in centrality classes measured by ALICE. The measurement covers a wide pseudorapidity range from $-3.5$ to $5$, which is sufficient for reliable estimates of the total number of charged particles produced in the collisions. For the most central collisions we find $21\,400\pm 1\,300$ while for the most peripheral we find $230\pm 38$. This corresponds to an increase of $(27\pm4)\%$ over the results at $\sqrt{s_{_{\mathrm{NN}}}}=2.76\,\mathrm{TeV}$ previously reported by ALICE. The energy dependence of the total number of charged particles produced in heavy-ion collisions is found to obey a modified power-law like behaviour. The charged-particle
pseudorapidity density of the most central collisions is compared to model calculations - none of which fully describes the measured distribution. We also present an estimate of the rapidity density of charged particles. The width of that distribution is found to exhibit a remarkable proportionality to the beam rapidity, independent of the collision energy from the top SPS to LHC energies.
DOI: 10.17182/hepdata.78365.v1/t3
title: "MULT" of "Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Total number of charged particles as a function of the mean number of participating nucleons [PRC88.044909]. The total charged-particle multiplicity is given as the integral over $\mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ over the measured region ($-3.5&lt;\eta&lt;5$) and extrapolations from fitted functions in the unmeasured regions. The contribution from unmeasured $\eta$ regions amounts to $\approx30\%$ of the total number of charged particles. The uncertainty on the extrapolation to the unmeasured pseudorapidity region is smaller than the size of the markers. The contribution to the systematic uncertainties from the centrality determination and electromagnetic processes are vanishing compared to the contribution from the largest differences between the fitted functions. A function inspired by factorisation [PRC83.024913] is fitted to the data, and the best fit yields $a=51.5\pm7.3$, $b=0.16\pm0.05$.
description: CERN-LHC. We present the charged-particle pseudorapidity density in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$ in centrality classes measured by ALICE. The measurement covers a wide pseudorapidity range from $-3.5$ to $5$, which is sufficient for reliable estimates of the total number of charged particles produced in the collisions. For the most central collisions we find $21\,400\pm 1\,300$ while for the most peripheral we find $230\pm 38$. This corresponds to an increase of $(27\pm4)\%$ over the results at $\sqrt{s_{_{\mathrm{NN}}}}=2.76\,\mathrm{TeV}$ previously reported by ALICE. The energy dependence of the total number of charged particles produced in heavy-ion collisions is found to obey a modified power-law like behaviour. The charged-particle
pseudorapidity density of the most central collisions is compared to model calculations - none of which fully describes the measured distribution. We also present an estimate of the rapidity density of charged particles. The width of that distribution is found to exhibit a remarkable proportionality to the beam rapidity, independent of the collision energy from the top SPS to LHC energies.
DOI: 10.5064/f6g2petf/w9zgyh
title: Moore-et-al_MD_0121_COVID-Vaccine-FactSheet_1.6_1500.pdf
DOI: 10.17182/hepdata.77359.v1/t5
title: "Table 5" of "W and Z boson production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Sum of the cross sections of positive and negative charge muons from W boson decays measured in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV in the negative rapidity region. The cross sections are normalised by the number of binary collisions $N_{\rm coll}$. The first uncertainty is statistical, the second is systematic and it does not include the global uncertainty (MB cross section, normalisation, acceptance times efficiency corrections and tracking and trigger systematics).
description: The W and Z boson production was measured via the muonic decay channel in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV at the Large Hadron Collider with the ALICE detector.
The measurement covers backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity regions, corresponding to Pb-going and p-going directions, respectively.
The Z-boson production cross section, with dimuon invariant mass of $6010$ GeV/$c$ are determined.
The W-boson production is also studied as a function of the collision centrality: the cross section of muons from W-boson decays is found to scale with the average number of binary nucleon-nucleon collisions within uncertainties.