cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.160246.v1/t10
title: "Figure 6" of "Charged-particle multiplicity distributions over a wide pseudorapidity range in p-Pb collisions at $\mathbf{\sqrt{s}_{NN} = 5.02}$ TeV"

description: Average charged-particle multiplicity normalised by the average number of participating nucleon pairs in NSD p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5020~\mathrm{GeV}$ for the pseudorapidity interval $-3.4&lt;\eta&lt;5.0$.
description: This paper presents the primary charged-particle multiplicity distributions in proton--lead collisions at a centre-of-mass energy per nucleon--nucleon collision of $\mathbf{\sqrt{\textit{s}_{\textup{NN}}} = 5.02}$ TeV. The distributions are reported for non-single diffractive collisions in different pseudorapidity ranges. The measurements are performed using the combined information from the Silicon Pixel Detector and the Forward Multiplicity Detector of ALICE. The multiplicity distributions are parametrised with a double negative binomial distribution function which provides satisfactory descriptions of the distributions for all the studied pseudorapidity intervals. The data are compared to models and analysed quantitatively, evaluating the first four moments (mean, standard deviation, skewness, and kurtosis). The shape evolution of the measured multiplicity distributions is studied in terms of KNO variables and it is found that none of the considered models reproduces the measurements. This paper also reports on the average charged-particle multiplicity, normalised by the average number of participating nucleon pairs, as a function of the collision energy. The multiplicity results are then compared to measurements made in proton--proton and nucleus--nucleus collisions across a wide range of collision energies.
DOI: 10.17182/hepdata.160246.v1/t6
title: "Figure 5 (open square symbol)" of "Charged-particle multiplicity distributions over a wide pseudorapidity range in p-Pb collisions at $\mathbf{\sqrt{s}_{NN} = 5.02}$ TeV"

description: KNO-scaled multiplicity distribution versus the KNO variable $N_{\rm ch}/\langle N_{\rm ch}\rangle$ in NSD p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5020~\mathrm{GeV}$ for the pseudorapidity interval $|\eta|&lt;3.4$.
description: This paper presents the primary charged-particle multiplicity distributions in proton--lead collisions at a centre-of-mass energy per nucleon--nucleon collision of $\mathbf{\sqrt{\textit{s}_{\textup{NN}}} = 5.02}$ TeV. The distributions are reported for non-single diffractive collisions in different pseudorapidity ranges. The measurements are performed using the combined information from the Silicon Pixel Detector and the Forward Multiplicity Detector of ALICE. The multiplicity distributions are parametrised with a double negative binomial distribution function which provides satisfactory descriptions of the distributions for all the studied pseudorapidity intervals. The data are compared to models and analysed quantitatively, evaluating the first four moments (mean, standard deviation, skewness, and kurtosis). The shape evolution of the measured multiplicity distributions is studied in terms of KNO variables and it is found that none of the considered models reproduces the measurements. This paper also reports on the average charged-particle multiplicity, normalised by the average number of participating nucleon pairs, as a function of the collision energy. The multiplicity results are then compared to measurements made in proton--proton and nucleus--nucleus collisions across a wide range of collision energies.
DOI: 10.17182/hepdata.160246.v1/t8
title: "Figure 5 (open triangle symbol)" of "Charged-particle multiplicity distributions over a wide pseudorapidity range in p-Pb collisions at $\mathbf{\sqrt{s}_{NN} = 5.02}$ TeV"

description: KNO-scaled multiplicity distribution versus the KNO variable $N_{\mathrm{ch}}/\langle N_{\mathrm{ch}}\rangle$ in NSD p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5020~\mathrm{GeV}$ for the pseudorapidity interval $-3.4&lt;\eta&lt;-1.0$.
description: This paper presents the primary charged-particle multiplicity distributions in proton--lead collisions at a centre-of-mass energy per nucleon--nucleon collision of $\mathbf{\sqrt{\textit{s}_{\textup{NN}}} = 5.02}$ TeV. The distributions are reported for non-single diffractive collisions in different pseudorapidity ranges. The measurements are performed using the combined information from the Silicon Pixel Detector and the Forward Multiplicity Detector of ALICE. The multiplicity distributions are parametrised with a double negative binomial distribution function which provides satisfactory descriptions of the distributions for all the studied pseudorapidity intervals. The data are compared to models and analysed quantitatively, evaluating the first four moments (mean, standard deviation, skewness, and kurtosis). The shape evolution of the measured multiplicity distributions is studied in terms of KNO variables and it is found that none of the considered models reproduces the measurements. This paper also reports on the average charged-particle multiplicity, normalised by the average number of participating nucleon pairs, as a function of the collision energy. The multiplicity results are then compared to measurements made in proton--proton and nucleus--nucleus collisions across a wide range of collision energies.
DOI: 10.17182/hepdata.160246.v1/t9
title: "Figure 5 (open cross symbol)" of "Charged-particle multiplicity distributions over a wide pseudorapidity range in p-Pb collisions at $\mathbf{\sqrt{s}_{NN} = 5.02}$ TeV"

description: KNO-scaled multiplicity distribution versus the KNO variable $N_{\mathrm{ch}}/\langle N_{\mathrm{ch}}\rangle$ in NSD p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5020~\mathrm{GeV}$ for the pseudorapidity interval $2.0&lt;\eta&lt;5.0$.
description: This paper presents the primary charged-particle multiplicity distributions in proton--lead collisions at a centre-of-mass energy per nucleon--nucleon collision of $\mathbf{\sqrt{\textit{s}_{\textup{NN}}} = 5.02}$ TeV. The distributions are reported for non-single diffractive collisions in different pseudorapidity ranges. The measurements are performed using the combined information from the Silicon Pixel Detector and the Forward Multiplicity Detector of ALICE. The multiplicity distributions are parametrised with a double negative binomial distribution function which provides satisfactory descriptions of the distributions for all the studied pseudorapidity intervals. The data are compared to models and analysed quantitatively, evaluating the first four moments (mean, standard deviation, skewness, and kurtosis). The shape evolution of the measured multiplicity distributions is studied in terms of KNO variables and it is found that none of the considered models reproduces the measurements. This paper also reports on the average charged-particle multiplicity, normalised by the average number of participating nucleon pairs, as a function of the collision energy. The multiplicity results are then compared to measurements made in proton--proton and nucleus--nucleus collisions across a wide range of collision energies.
DOI: 10.17182/hepdata.168550.v1/t1
title: "Table 1" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class I, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t2
title: "Table 2" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class II, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t3
title: "Table 3" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class III, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t4
title: "Table 4" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class IV+V, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t5
title: "Table 5" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class VI, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t6
title: "Table 6" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class VII, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t7
title: "Table 7" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class VIII, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t11
title: "Table 11" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class II
description: .
DOI: 10.17182/hepdata.168550.v1/t15
title: "Table 15" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class VII
description: .
DOI: 10.17182/hepdata.168550.v1/t8
title: "Table 8" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class IX, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t9
title: "Table 9" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum - V0M multiplicity class X, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t10
title: "Table 10" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class I
description: .
DOI: 10.17182/hepdata.168550.v1/t12
title: "Table 12" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class III
description: .
DOI: 10.17182/hepdata.168550.v1/t13
title: "Table 13" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class IV+V
description: .
DOI: 10.17182/hepdata.168550.v1/t14
title: "Table 14" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class VI
description: .
DOI: 10.17182/hepdata.168550.v1/t16
title: "Table 16" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class VIII
description: .
DOI: 10.17182/hepdata.168550.v1/t17
title: "Table 17" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class IX
description: .
DOI: 10.17182/hepdata.168550.v1/t18
title: "Table 18" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum spectrum ratio to INEL&gt;0 - V0M multiplicity class X
description: .
DOI: 10.17182/hepdata.168550.v1/t19
title: "Table 19" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ transverse momentum integrated yield vs multiplicity - V0M multiplicity classes, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t20
title: "Table 20" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$ average transverse momentum vs multiplicity - V0M multiplicity classes, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t21
title: "Table 21" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$/K$_{\mathrm{S}}^{0}$ transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t22
title: "Table 22" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\PM}$/K$_{\mathrm{S}}^{0}$ yield ratio vs transverse momentum - V0M multiplicity class I, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t23
title: "Table 23" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\PM}$/K$_{\mathrm{S}}^{0}$ yield ratio vs transverse momentum - V0M multiplicity class X, average of particle and antiparticle
description: .
DOI: 10.17182/hepdata.168550.v1/t24
title: "Table 24" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: K$^{*\pm}$/K$_{\mathrm{S}}^{0}$ double yield ratio vs transverse momentum - V0M multiplicity class I / V0M multiplicity class X, average of particle and antiparticle
description: .
DOI: 10.57996/cran.ceres-2667
title: Dataset: Using model compounds to show how a change in thinking is required for regulation of brominated haloacetic acids in drinking water

description: This project looks at the Disinfection By-Products (DBPs) formed from model compounds during their chlorination with bromide present. This data set is the results obtained from the analysis for trihalomethanes (THMs) and haloacetic acids (HAAs).
DOI: 10.17182/hepdata.157865.v1/t1
title: "Table 1" of "Measurement of $\omega$ meson production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Invariant differential cross section of OMEGA mesons produced in inelastic pp collisions at center-of-mass energy 13 TeV, the uncertainty of sigma_{MB} of 1.58% is not included in the systematic error.
description: CERN-LHC. The $p_{\rm T}$-differential cross section of $\omega$ meson production in pp collisions at $\sqrt{s}=13$ TeV at midrapidity ($|y|&lt;0.5$) was measured with the ALICE detector at the LHC, covering an unprecedented transverse-momentum range of $1.6
DOI: 10.17182/hepdata.165812.v1/t1
title: "Figure 1 left, panel a" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: proton-proton (same charge) correlation function for centrality 0-10% from 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/t2
title: "Figure 1 centre, panel b" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: proton-proton (same charge) correlation function for centrality 10-30% from 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/t3
title: "Figure 1 right, panel c" of "Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHC"

description: proton-proton (same charge) correlation function for centrality 30-50% from 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.168550.v1/t25
title: "Table 25" of "Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Significance of K$^{*\pm}$/K$_{\mathrm{S}}^{0}$ double yield ratio vs transverse momentum - V0M multiplicity class I / V0M multiplicity class X
description: .
DOI: 10.17182/hepdata.157865.v1/t2
title: "Table 2" of "Measurement of $\omega$ meson production in pp collisions at $\sqrt{s}$ = 13 TeV"

description: The measured ratio of cross sections for inclusive OMEGA to PI0 production at a centre-of-mass energy of 13 TeV.
description: CERN-LHC. The $p_{\rm T}$-differential cross section of $\omega$ meson production in pp collisions at $\sqrt{s}=13$ TeV at midrapidity ($|y|&lt;0.5$) was measured with the ALICE detector at the LHC, covering an unprecedented transverse-momentum range of $1.6
DOI: 10.17182/hepdata.165812.v1/t4
title: "Figure 2, left, protons $0-10\%$" 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 $0-10\%$ 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.