cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.165812.v1/t5
title: "Figure 2, left, protons $10-30\%$" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm p}$ vs. $m_{\rm T}$ for $10-30\%$ centrality for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t6
title: "Figure 2, left, protons $30-50\%$" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm p}$ vs. $m_{\rm T}$ for $30-50\%$ centrality for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t10
title: "Figure 2, left, deuterons $0-10\%$" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm d}$ vs. $m_{\rm T}$ for $0-10\%$ centrality for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t11
title: "Figure 2, left, deuterons $10-30\%$" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm d}$ vs. $m_{\rm T}$ for $10-30\%$ centrality for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t12
title: "Figure 2, left, deuterons $30-50\%$" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm d}$ vs. $m_{\rm T}$ for $30-50\%$ centrality for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t13
title: "Figure 2, right, protons mT bin 0" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm p}$ vs. '^{1/3}' for mT bin 0 for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t14
title: "Figure 2, right, protons mT bin 1" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm p}$ vs. '^{1/3}' for mT bin 1 for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t7
title: "Figure 2, left, nucleons $0-10\%$" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm N}$ vs. $m_{\rm T}$ for $0-10\%$ centrality for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t8
title: "Figure 2, left, nucleons $10-30\%$" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm N}$ vs. $m_{\rm T}$ for $10-30\%$ centrality for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t9
title: "Figure 2, left, nucleons $30-50\%$" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm N}$ vs. $m_{\rm T}$ for $30-50\%$ centrality for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t15
title: "Figure 2, right, protons mT bin 2" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm p}$ vs. '^{1/3}' for mT bin 2 for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t16
title: "Figure 2, right, protons mT bin 3" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm p}$ vs. '^{1/3}' for mT bin 3 for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.
DOI: 10.17182/hepdata.165812.v1/t17
title: "Figure 2, right, protons mT bin 4" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: $R_{\rm p}$ vs. '^{1/3}' for mT bin 4 for Pb-Pb collisions at 5020 GeV.
description: This work reports femtoscopy correlations of $p-p (\overline{p}-\overline{p})$ and $p-d (\overline{p}-\overline{d})$ pairs measured in Pb--Pb collisions at center-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02~TeV by the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source as a function of the pair transverse mass ($m_\text{T}$) and of the average charge particle multiplicity $\langle\text{dN}_\text{ch}/\text{d}\eta\rangle^{1/3}$ for three centrality intervals (0--10$\%$, 10--30$\%$, 30--50$\%$). In both cases, the expected power-law and liner scalings are observed, respectively. The measured \pd correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in \mbox{Pb--Pb} collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons start at $2.73^{+0.05}_{-0.05}$ and $3.10^{+1.04}_{-0.86}$~fm, respectively, for the 30–50$\%$ centrality of the collisions. Moreover, the $m_{\rm{T}}$-scaling obtained for the \pP and \pd systems is compatible within 1$\sigma$ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.