cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.137818.v1/t2
title: "Table 2" of "System-size dependence of the charged-particle pseudorapidity density at $\sqrt{s_{\rm NN}} = 5.02$ TeV for pp, p-Pb, and Pb-Pb collisions"

description: $\frac{\mathrm{d}N}{\mathrm{d}\eta}$ versus $\eta$ for $x^{\pm}$ in $\mathrm{p}-\mathrm{Pb}$ at $\sqrt{s_{\mathrm{NN}}}=5.023\,\mathrm{Te\!V}$
description: ALICE. We present and compare the charged-particle pseudorapidity densities for pp, p-Pb, and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV measured over a wide pseudorapidity range (${-3.5 &lt;\eta &lt;5}$), using ALICE at the Large Hadron Collider. The distributions for p-Pb and Pb-Pb collisions are determined as a function of the centrality of the collisions, while results from pp collisions are reported for inelastic events with at least one charged particle at midrapidity. The charged-particle pseudorapidity densities are, under simple and robust assumptions, transformed to charged-particle rapidity densities. This allows for the calculation and the presentation of the evolution of the width of the rapidity distributions and of a lower bound on the Bjorken energy density, as a function of the number of participants in all three collision systems. We find a decreasing width of the particle production, and roughly a ten fold increase in the energy density, as the system size grows.
DOI: 10.17182/hepdata.137818.v1/t4
title: "Table 4" of "System-size dependence of the charged-particle pseudorapidity density at $\sqrt{s_{\rm NN}} = 5.02$ TeV for pp, p-Pb, and Pb-Pb collisions"

description: $N_{\mathrm{ch}}^{\mathrm{tot}}$, $p_{\mathrm{T}}/m$, $\varepsilon_{\mathrm{LB}}^{\cap}\tau$, $\varepsilon_{\mathrm{LB}}^{\cup}\tau$, $N_{\mathrm{part}}$, $S_{\mathrm{T}}^{\cup}$, $S_{\mathrm{T}}^{\cap}$, $\sigma_{\mathrm{d}N/{\mathrm{d}y}}$ versus $\mathrm{Centrality}$ for $x^{\pm}$, $x_{\mathrm{primary}}$, $\mathrm{participant}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=5.023\,\mathrm{Te\!V}$
description: ALICE. We present and compare the charged-particle pseudorapidity densities for pp, p-Pb, and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV measured over a wide pseudorapidity range (${-3.5 &lt;\eta &lt;5}$), using ALICE at the Large Hadron Collider. The distributions for p-Pb and Pb-Pb collisions are determined as a function of the centrality of the collisions, while results from pp collisions are reported for inelastic events with at least one charged particle at midrapidity. The charged-particle pseudorapidity densities are, under simple and robust assumptions, transformed to charged-particle rapidity densities. This allows for the calculation and the presentation of the evolution of the width of the rapidity distributions and of a lower bound on the Bjorken energy density, as a function of the number of participants in all three collision systems. We find a decreasing width of the particle production, and roughly a ten fold increase in the energy density, as the system size grows.
DOI: 10.17182/hepdata.137818.v1/t6
title: "Table 6" of "System-size dependence of the charged-particle pseudorapidity density at $\sqrt{s_{\rm NN}} = 5.02$ TeV for pp, p-Pb, and Pb-Pb collisions"

description: $N_{\mathrm{ch}}^{\mathrm{tot}}$, $p_{\mathrm{T}}/m$, $\varepsilon_{\mathrm{LB}}^{\cap}\tau$, $\varepsilon_{\mathrm{LB}}^{\cup}\tau$, $N_{\mathrm{part}}$, $S_{\mathrm{T}}^{\cup}$, $S_{\mathrm{T}}^{\cap}$, $\sigma_{\mathrm{d}N/{\mathrm{d}y}}$ versus $\mathrm{Centrality}$ for $x^{\pm}$, $x_{\mathrm{primary}}$, $\mathrm{participant}$ in $\mathrm{Pb}-\mathrm{Pb}$ at $\sqrt{s_{\mathrm{NN}}}=5.023\,\mathrm{Te\!V}$
description: ALICE. We present and compare the charged-particle pseudorapidity densities for pp, p-Pb, and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV measured over a wide pseudorapidity range (${-3.5 &lt;\eta &lt;5}$), using ALICE at the Large Hadron Collider. The distributions for p-Pb and Pb-Pb collisions are determined as a function of the centrality of the collisions, while results from pp collisions are reported for inelastic events with at least one charged particle at midrapidity. The charged-particle pseudorapidity densities are, under simple and robust assumptions, transformed to charged-particle rapidity densities. This allows for the calculation and the presentation of the evolution of the width of the rapidity distributions and of a lower bound on the Bjorken energy density, as a function of the number of participants in all three collision systems. We find a decreasing width of the particle production, and roughly a ten fold increase in the energy density, as the system size grows.
DOI: 10.17182/hepdata.134042.v1/t6
title: "Table 6" of "$\Sigma(1385)^{\pm}$ resonance production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*-}$ + cc in Pb-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (50-90% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ produced in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.134042.v1/t9
title: "Table 9" of "$\Sigma(1385)^{\pm}$ resonance production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Mean $p_{\rm T}$ of ($\Sigma^{*+}+\overline{\Sigma}^{*-}$) in Pb-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ produced in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.138430.v1/t1
title: "Table1_1" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle correlation method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the V0M estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t2
title: "Table1_2" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the V0M estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t3
title: "Table1_3" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle correlation method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the V0M estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t4
title: "Table1_4" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the V0M estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.142594.v1/t1
title: "$z_{g}$" of "Measurements of groomed-jet substructure of charm jets tagged by ${\rm D}^0$ mesons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $z_{g}$ variable for $D^{0}$-tagged jets and non-flavour tagged jets in the $p_{T}^{jet ch}$: 15-30 GeV/$c$ interval.
description: Understanding the role of parton mass and Casimir colour factors in the quantum chromodynamics parton shower represents an important step in characterising the emission properties of heavy quarks. Recent experimental advances in jet substructure techniques have provided the opportunity to isolate and characterise gluon emissions from heavy quarks. In this work, the first direct experimental constraint on the charm-quark splitting function is presented, obtained via the measurement of the groomed shared momentum fraction of the first splitting in charm jets, tagged by a reconstructed D$^{0}$ meson. The measurement is made in proton--proton collisions at $\sqrt{s} = 13$ TeV, in the low jet transverse-momentum interval of $15 \leq p_{\rm{T}}^{jet ch} &lt; 30$ GeV/$c$ where the emission properties are sensitive to parton mass effects. In addition, the opening angle of the first perturbative emission of the charm quark, as well as the number of perturbative emissions it undergoes, are reported. Comparisons to measurements of an inclusive-jet sample show a steeper splitting function for charm quarks compared to gluons and light quarks. Charm quarks also undergo fewer perturbative emissions in the parton shower, with a reduced probability of large-angle emissions.
DOI: 10.17182/hepdata.144824.v1/t10
title: "Table 10" of "Higher-order correlations between different moments of two flow amplitudes in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Centrality dependence of ${\rm NAC}_{3,1}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: The correlations between different moments of two flow amplitudes, extracted with the recently developed asymmetric cumulants, are measured in Pb$-$Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV recorded by the ALICE detector at the LHC. The magnitudes of the measured observables show a dependence on the different moments as well as on the collision centrality, indicating the presence of non-linear response in all even moments up to the eighth. Furthermore, the higher-order asymmetric cumulants show different signatures than the symmetric and lower-order asymmetric cumulants. Comparisons with state-of-the-art event generators using two different parameterizations obtained from Bayesian optimization show differences between data and simulations in many of the studied observables, indicating a need for further tuning of the models behind those event generators. These results provide new and independent constraints on the initial conditions and transport properties of the system created in heavy-ion collisions.
DOI: 10.17182/hepdata.144824.v1/t11
title: "Table 11" of "Higher-order correlations between different moments of two flow amplitudes in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Centrality dependence of ${\rm NAC}_{1,3}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: The correlations between different moments of two flow amplitudes, extracted with the recently developed asymmetric cumulants, are measured in Pb$-$Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV recorded by the ALICE detector at the LHC. The magnitudes of the measured observables show a dependence on the different moments as well as on the collision centrality, indicating the presence of non-linear response in all even moments up to the eighth. Furthermore, the higher-order asymmetric cumulants show different signatures than the symmetric and lower-order asymmetric cumulants. Comparisons with state-of-the-art event generators using two different parameterizations obtained from Bayesian optimization show differences between data and simulations in many of the studied observables, indicating a need for further tuning of the models behind those event generators. These results provide new and independent constraints on the initial conditions and transport properties of the system created in heavy-ion collisions.
DOI: 10.17182/hepdata.134042.v1/t10
title: "Table 10" of "$\Sigma(1385)^{\pm}$ resonance production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Mean $p_{\rm T}$ of ($\Sigma^{*-}+\overline{\Sigma}^{*+}$) in Pb-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ produced in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.134042.v1/t11
title: "Table 11" of "$\Sigma(1385)^{\pm}$ resonance production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Integrated yield ratio.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ produced in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.134042.v1/t8
title: "Table 8" of "$\Sigma(1385)^{\pm}$ resonance production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: $p_{\rm T}$-integrated yield d$N$/d$y$ of ($\Sigma^{*-}+\overline{\Sigma}^{*+}$) in Pb-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ produced in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.138430.v1/t11
title: "Table2_7" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle corrrelation method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the CL1 estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t5
title: "Table2_1" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the CL1 estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t9
title: "Table2_5" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle correlation method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the CL1 estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.145654.v1/t3
title: "Table 3" of "$\psi(2S)$ suppression in Pb-Pb collisions at the LHC"

description: Nuclear modification factor of the $\psi$(2S) shown as a function of centrality
description: CERN-LHC-ALICE. The production of the $\psi(2S)$ charmonium state was measured with ALICE in Pb--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV, in the dimuon decay channel. A significant signal was observed for the first time at LHC energies down to zero transverse momentum, at forward rapidity ($2.5
DOI: 10.5281/zenodo.17504146
title: Datos del diagnóstico de las personas creadoras y promotoras culturales independientes del municipio de Guadalajara (2025)

description: Data generated from the questionnaire applied to municipal cultural spaces and the participatory diagnosis. They allow characterization of spaces and analysis of sustainability, networks, and cultural participation.
description: Datos generados a partir del cuestionario aplicado a los espacios culturales municipales y del diagnóstico participativo. Permiten caracterizar espacios y analizar sostenibilidad, redes y participación cultural.
description: Dados gerados a partir do questionário aplicado aos espaços culturais municipais e do diagnóstico participativo. Permitem caracterizar espaços e analisar sustentabilidade, redes e participação cultural.