cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.78549.v1/t4
title: "Table 4" of "Measurement of deuteron spectra and elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 2.76 TeV at the LHC"

description: v2 of anti-deuterons and deuterons vs $p_{\mathrm T}$ for different centrality intervals
description: The transverse momentum ($p_{\mathrm{T}}$) spectra and elliptic flow coefficient ($v_{2}$) of deuterons and anti-deuterons at mid-rapidity ($|y|&lt;0.5$) are measured with the ALICE detector at the LHC in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV. The measurement of the $p_{\mathrm{T}}$ spectra of (anti-)deuterons is done up to 8 GeV/$c$ in 0-10\% centrality class and up to 6 GeV/$c$ in 10-20\% and 20-40\% centrality classes. The $v_{2}$ is measured in the 0.8 $&lt;$ $p_{\mathrm{T}}$ $&lt; $5 GeV/$c$ interval and in six different centrality intervals (0-5\%, 5-10\%, 10-20\%, 20-30\%, 30-40\% and 40-50\%) using the scalar product technique. Measured \pio$^{\pm}$, K$^{\pm}$ and p+$\overline{\mathrm{p}}$ transverse-momentum spectra and $v_{2}$ are used to predict the deuteron $p_{\mathrm{T}}$ spectra and $v_{2}$ within the Blast-Wave model. The predictions are able to reproduce the $v_{2}$ coefficient in the measured $p_{\mathrm{T}}$ range and the transverse-momentum spectra for $p_{\mathrm{T}}$ $&gt;$ 1.8 GeV/$c$ within the experimental uncertainties. The measurement of the coalescence parameter $B_2$ is performed, showing a $p_{\mathrm{T}}$ dependence in contrast with the simplest coalescence model, which fails to reproduce also the measured $v_{2}$ coefficient. In addition, the coalescence parameter $B_2$ and the elliptic flow coefficient in the 20-40\% centrality interval are compared with the AMPT model which is able, in its version without string melting, to reproduce the measured $v_{2}$($p_{\mathrm{T}}$) and the $B_2$($p_{\mathrm{T}}$) trend.
DOI: 10.17182/hepdata.78549.v1/t5
title: "Table 5" of "Measurement of deuteron spectra and elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 2.76 TeV at the LHC"

description: $B_2$ vs $p_{\mathrm T/A}$ for $p_{\mathrm T/A} &gt; $ 2.2 GeV/$c$. Low $p_{\mathrm T/A}$ points can be found here 'http://hepdata.cedar.ac.uk/view/ins1380491'
description: The transverse momentum ($p_{\mathrm{T}}$) spectra and elliptic flow coefficient ($v_{2}$) of deuterons and anti-deuterons at mid-rapidity ($|y|&lt;0.5$) are measured with the ALICE detector at the LHC in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV. The measurement of the $p_{\mathrm{T}}$ spectra of (anti-)deuterons is done up to 8 GeV/$c$ in 0-10\% centrality class and up to 6 GeV/$c$ in 10-20\% and 20-40\% centrality classes. The $v_{2}$ is measured in the 0.8 $&lt;$ $p_{\mathrm{T}}$ $&lt; $5 GeV/$c$ interval and in six different centrality intervals (0-5\%, 5-10\%, 10-20\%, 20-30\%, 30-40\% and 40-50\%) using the scalar product technique. Measured \pio$^{\pm}$, K$^{\pm}$ and p+$\overline{\mathrm{p}}$ transverse-momentum spectra and $v_{2}$ are used to predict the deuteron $p_{\mathrm{T}}$ spectra and $v_{2}$ within the Blast-Wave model. The predictions are able to reproduce the $v_{2}$ coefficient in the measured $p_{\mathrm{T}}$ range and the transverse-momentum spectra for $p_{\mathrm{T}}$ $&gt;$ 1.8 GeV/$c$ within the experimental uncertainties. The measurement of the coalescence parameter $B_2$ is performed, showing a $p_{\mathrm{T}}$ dependence in contrast with the simplest coalescence model, which fails to reproduce also the measured $v_{2}$ coefficient. In addition, the coalescence parameter $B_2$ and the elliptic flow coefficient in the 20-40\% centrality interval are compared with the AMPT model which is able, in its version without string melting, to reproduce the measured $v_{2}$($p_{\mathrm{T}}$) and the $B_2$($p_{\mathrm{T}}$) trend.
DOI: 10.5064/f6g2petf/a7zsok
title: Moore-et-al_MD_0221_Governor Larry Hogan - Official Website for the Governor of Maryland_12.pdf
DOI: 10.17182/hepdata.78255.v1/t3
title: "Table 3" of "D-meson azimuthal anisotropy in mid-central Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV"

description: $v_2$ vs. $p_{\rm T}$ of $D^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=5.02 TeV in the centrality class 30-50% in the rapidity interval |$y$|&lt;0.8.
The second (sys) error is the systematic uncertainty from the B feed-down contribution.
The first (sys) error is the systematic uncertainty from the other sources.
description: CERN-LHC. The azimuthal anisotropy coefficient $v_2$ of prompt $D^0$, $D^+$, $D^{*+}$ and $D_s^+$ mesons was measured in mid-central (30-50% centrality class) Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}$ = 5.02 TeV, with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays at mid-rapidity, |$y$|&lt;0.8, in the transverse momentum interval 1&lt;$p_{\rm T}$&lt;24 GeV/$c$. The measured D-meson $v_2$ has similar values as that of charged pions. The $D_s^+$ $v_2$, measured for the first time, is found to be compatible with that of non-strange D mesons. The measurements are compared with theoretical calculations of charm-quark transport in a hydrodynamically expanding medium and have the potential to constrain medium parameters.
DOI: 10.17182/hepdata.78255.v1/t4
title: "Table 4" of "D-meson azimuthal anisotropy in mid-central Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV"

description: $v_2$ vs. $p_{\rm T}$ of $D_s^+$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=5.02 TeV in the centrality class 30-50% in the rapidity interval |$y$|&lt;0.8.
The second (sys) error is the systematic uncertainty from the B feed-down contribution.
The first (sys) error is the systematic uncertainty from the other sources.
description: CERN-LHC. The azimuthal anisotropy coefficient $v_2$ of prompt $D^0$, $D^+$, $D^{*+}$ and $D_s^+$ mesons was measured in mid-central (30-50% centrality class) Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}$ = 5.02 TeV, with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays at mid-rapidity, |$y$|&lt;0.8, in the transverse momentum interval 1&lt;$p_{\rm T}$&lt;24 GeV/$c$. The measured D-meson $v_2$ has similar values as that of charged pions. The $D_s^+$ $v_2$, measured for the first time, is found to be compatible with that of non-strange D mesons. The measurements are compared with theoretical calculations of charm-quark transport in a hydrodynamically expanding medium and have the potential to constrain medium parameters.
DOI: 10.17182/hepdata.78255.v1/t5
title: "Table 5" of "D-meson azimuthal anisotropy in mid-central Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV"

description: $v_2$ vs. $p_{\rm T}$ of $D^0$, $D^+$, $D^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=5.02 TeV in the centrality class 30-50% in the rapidity interval |$y$|&lt;0.8.
The second (sys) error is the systematic uncertainty from the B feed-down contribution.
The first (sys) error is the systematic uncertainty from the other sources.
description: CERN-LHC. The azimuthal anisotropy coefficient $v_2$ of prompt $D^0$, $D^+$, $D^{*+}$ and $D_s^+$ mesons was measured in mid-central (30-50% centrality class) Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}$ = 5.02 TeV, with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays at mid-rapidity, |$y$|&lt;0.8, in the transverse momentum interval 1&lt;$p_{\rm T}$&lt;24 GeV/$c$. The measured D-meson $v_2$ has similar values as that of charged pions. The $D_s^+$ $v_2$, measured for the first time, is found to be compatible with that of non-strange D mesons. The measurements are compared with theoretical calculations of charm-quark transport in a hydrodynamically expanding medium and have the potential to constrain medium parameters.
DOI: 10.17182/hepdata.80256.v1/t1
title: "Table 1" of "J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Relative yield of inclusive J/psi mesons as a function of relative charged-particle pseudorapidity density for forward rapidities 2.03 &lt; y_cms &lt; 3.53 (p-going direction).
description: No data abstract available.
DOI: 10.17182/hepdata.80256.v1/t2
title: "Table 2" of "J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Relative yield of inclusive J/psi mesons as a function of relative charged-particle pseudorapidity density for backward rapidities -4.46 &lt; y_cms &lt; -2.96 (Pb-going direction).
description: No data abstract available.
DOI: 10.17182/hepdata.80256.v1/t3
title: "Table 3" of "J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Relative yield of inclusive J/psi mesons as a function of relative charged-particle pseudorapidity density for central rapidities -1.37 &lt; y_cms &lt; 0.43.
description: No data abstract available.
DOI: 10.17182/hepdata.80256.v1/t4
title: "Table 4" of "J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: RFB of inclusive JPSI(1S) in p-Pb collisions as a function of relative charged-particle pseudorapidity density.
description: No data abstract available.
DOI: 10.17182/hepdata.80256.v1/t5
title: "Table 5" of "J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Relative mean transverse momentum of JPSI(1S) mesons for backward rapidity as a function of the relative charged-particle pseudorapidity density.
description: No data abstract available.
DOI: 10.17182/hepdata.80256.v1/t6
title: "Table 6" of "J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Relative mean transverse momentum of JPSI(1S) mesons for forward rapidity as a function of the relative charged-particle pseudorapidity density.
description: No data abstract available.
DOI: 10.5064/f6g2petf/tszcqf
title: Moore-et-al_ME_0421_ADVISORY_ Maine Advises Pause for Johnson and Johnson COVID-19 Vaccine _ Office of Governor Janet T. Mills.pdf
DOI: 10.17182/hepdata.77600.v1/t1
title: "Table 1" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

description: pT-differential production cross section of heavy-flavour decay muons at forward rapidity (proton-going side) and backward rapidity (Pb-going side)
description: CERN-LHC. The production of muons from heavy-flavour hadron decays in p--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$~TeV was studied for $2
DOI: 10.17182/hepdata.79044.v1/t1
title: "Table 1" of "$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV"

description: Invariant differential cross section of $\pi^0$ produced in inelastic pp collisions at center-of-mass energy 8 TeV, the uncertainty of $\sigma_{MB}$ of 2.6% is not included in the systematic error.
description: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^0$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$ TeV was carried out by the ALICE experiment at the LHC. The spectra of neutral mesons $\pi^0$ and $\eta$ were measured in transverse momentum ranges of $0.33.5$ GeV/$c$. However, a deviation from this empirical scaling law is observed for transverse momenta below $p_{\rm T}&lt;3.5$ GeV/$c$ in the $\eta$/$\pi^0$ ratio with a significance of $6.2\sigma$.
DOI: 10.17182/hepdata.79044.v1/t2
title: "Table 2" of "$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV"

description: Invariant differential cross section of $\eta$ produced in inelastic pp collisions at center-of-mass energy 8 TeV, the uncertainty of $\sigma_{MB}$ of 2.6% is not included in the systematic error.
description: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^0$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$ TeV was carried out by the ALICE experiment at the LHC. The spectra of neutral mesons $\pi^0$ and $\eta$ were measured in transverse momentum ranges of $0.33.5$ GeV/$c$. However, a deviation from this empirical scaling law is observed for transverse momenta below $p_{\rm T}&lt;3.5$ GeV/$c$ in the $\eta$/$\pi^0$ ratio with a significance of $6.2\sigma$.
DOI: 10.17182/hepdata.77600.v1/t2
title: "Table 2" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

description: pT-differential nuclear modification factor of heavy-flavour decay muons at forward rapidity (proton-going side)
description: CERN-LHC. The production of muons from heavy-flavour hadron decays in p--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$~TeV was studied for $2
DOI: 10.17182/hepdata.77600.v1/t3
title: "Table 3" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

description: pT-differential nuclear modification factor of heavy-flavour decay muons at backward rapidity (Pb-going side)
description: CERN-LHC. The production of muons from heavy-flavour hadron decays in p--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$~TeV was studied for $2
DOI: 10.17182/hepdata.79044.v1/t3
title: "Table 3" of "$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV"

description: Integrated yields of $\pi^0$ mesons produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV. The uncertainties of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV are not included in the systematic error.
description: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^0$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$ TeV was carried out by the ALICE experiment at the LHC. The spectra of neutral mesons $\pi^0$ and $\eta$ were measured in transverse momentum ranges of $0.33.5$ GeV/$c$. However, a deviation from this empirical scaling law is observed for transverse momenta below $p_{\rm T}&lt;3.5$ GeV/$c$ in the $\eta$/$\pi^0$ ratio with a significance of $6.2\sigma$.
DOI: 10.17182/hepdata.79044.v1/t4
title: "Table 4" of "$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV"

description: Integrated yields of $\eta$ mesons produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV. The uncertainties of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV are not included in the systematic error.
description: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^0$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$ TeV was carried out by the ALICE experiment at the LHC. The spectra of neutral mesons $\pi^0$ and $\eta$ were measured in transverse momentum ranges of $0.33.5$ GeV/$c$. However, a deviation from this empirical scaling law is observed for transverse momenta below $p_{\rm T}&lt;3.5$ GeV/$c$ in the $\eta$/$\pi^0$ ratio with a significance of $6.2\sigma$.
DOI: 10.17182/hepdata.79044.v1/t5
title: "Table 5" of "$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV"

description: Integrated $\eta$/$\pi^0$ ratio produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV.
description: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^0$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$ TeV was carried out by the ALICE experiment at the LHC. The spectra of neutral mesons $\pi^0$ and $\eta$ were measured in transverse momentum ranges of $0.33.5$ GeV/$c$. However, a deviation from this empirical scaling law is observed for transverse momenta below $p_{\rm T}&lt;3.5$ GeV/$c$ in the $\eta$/$\pi^0$ ratio with a significance of $6.2\sigma$.
DOI: 10.17182/hepdata.77600.v1/t4
title: "Table 4" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

description: pT-differential nuclear modification factor of heavy-flavour decay muons at forward rapidity (proton-going side)
description: CERN-LHC. The production of muons from heavy-flavour hadron decays in p--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$~TeV was studied for $2
DOI: 10.17182/hepdata.77600.v1/t5
title: "Table 5" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

description: pT-differential nuclear modification factor of heavy-flavour decay muons at backward rapidity (Pb-going side)
description: CERN-LHC. The production of muons from heavy-flavour hadron decays in p--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$~TeV was studied for $2
DOI: 10.17182/hepdata.79044.v1/t6
title: "Table 6" of "$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV"

description: Mean transverse momenta $\langle p_\text{T}\rangle$ of $\pi^0$ mesons produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV. The uncertainties of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV are not included in the systematic error.
description: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^0$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$ TeV was carried out by the ALICE experiment at the LHC. The spectra of neutral mesons $\pi^0$ and $\eta$ were measured in transverse momentum ranges of $0.33.5$ GeV/$c$. However, a deviation from this empirical scaling law is observed for transverse momenta below $p_{\rm T}&lt;3.5$ GeV/$c$ in the $\eta$/$\pi^0$ ratio with a significance of $6.2\sigma$.
DOI: 10.17182/hepdata.79044.v1/t7
title: "Table 7" of "$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV"

description: Mean transverse momenta $\langle p_\text{T}\rangle$ of $\eta$ mesons produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV. The uncertainties of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV are not included in the systematic error.
description: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^0$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$ TeV was carried out by the ALICE experiment at the LHC. The spectra of neutral mesons $\pi^0$ and $\eta$ were measured in transverse momentum ranges of $0.33.5$ GeV/$c$. However, a deviation from this empirical scaling law is observed for transverse momenta below $p_{\rm T}&lt;3.5$ GeV/$c$ in the $\eta$/$\pi^0$ ratio with a significance of $6.2\sigma$.
DOI: 10.5064/f6g2petf/ap8i6m
title: Moore-et-al_ME_0821_Q&A webinar 7.29.21.pdf
DOI: 10.17182/hepdata.77600.v1/t6
title: "Table 6" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

description: pT-differential forward-to-backward ratio of heavy-flavour decay muons
description: CERN-LHC. The production of muons from heavy-flavour hadron decays in p--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$~TeV was studied for $2
DOI: 10.17182/hepdata.79044.v1/t8
title: "Table 8" of "$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV"

description: The measured ratio of cross sections for inclusive $\eta$ to $\pi^0$ production at a centre-of-mass energy of 8 TeV.
description: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^0$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$ TeV was carried out by the ALICE experiment at the LHC. The spectra of neutral mesons $\pi^0$ and $\eta$ were measured in transverse momentum ranges of $0.33.5$ GeV/$c$. However, a deviation from this empirical scaling law is observed for transverse momenta below $p_{\rm T}&lt;3.5$ GeV/$c$ in the $\eta$/$\pi^0$ ratio with a significance of $6.2\sigma$.
DOI: 10.17182/hepdata.79128.v1/t1
title: "Figure 2a" of "Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Out projection of raw 3D LCMS K+- K+- correlation function for 0.2 &lt; kT &lt; 0.4 GeV/c bin.
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/t2
title: "Figure 2b" of "Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Side projection of raw 3D LCMS K+- K+- correlation function for 0.2 &lt; kT &lt; 0.4 GeV/c bin
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.