cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.137819.v1/t22
title: "Figure 5.2" of "Two-particle transverse momentum correlations in pp and p-Pb collisions at LHC energies"

description: Evolution with the average charged particle multiplicity of the azimuthal widths of the two-particle transverse momentum differential correlation $G_{2}^{\rm CD}$ in pp and p$-$Pb collisions at $\sqrt{s} = 7\;\text{TeV}$ and $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$, respectively. Vertical bars (mostly smaller than the marker size) and filled boxes represent statistical and systematic uncertainties, respectively.
description: Two-particle transverse momentum differential correlators, recently measured in Pb$-$Pb collisions at LHC energies, provide an additional tool to gain insights into particle production mechanisms and infer transport properties, such as the ratio of shear viscosity to entropy density, of the medium created in Pb$-$Pb collisions. The longitudinal long-range correlations and the large azimuthal anisotropy measured at low transverse momenta in small collision systems, namely pp and p$-$Pb, at LHC energies resemble manifestations of collective behaviour. This suggests that locally equilibrated matter may be produced in these small collision systems, similar to what is observed in Pb$-$Pb collisions. In this work, the same two-particle transverse momentum differential correlators are exploited in pp and p$-$Pb collisions at $\sqrt{s} = 7\;\text{TeV}$ and $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$, respectively, to seek evidence for viscous effects. Specifically, the strength and shape of the correlators are studied as a function of the produced particle multiplicity to identify evidence for longitudinal broadening that might reveal the presence of viscous effects in these smaller systems. The measured correlators and their evolution from pp and p$-$Pb to Pb$-$Pb collisions are additionally compared to predictions from Monte Carlo event generators, and the potential presence of viscous effects is discussed.
DOI: 10.17182/hepdata.137819.v1/t23
title: "Figure 5.3" of "Two-particle transverse momentum correlations in pp and p-Pb collisions at LHC energies"

description: Evolution with the average charged particle multiplicity of the longitudinal widths of the two-particle transverse momentum differential correlation $G_{2}^{\rm CI}$ in pp and p$-$Pb collisions at $\sqrt{s} = 7\;\text{TeV}$ and $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$, respectively. Vertical bars (mostly smaller than the marker size) and filled boxes represent statistical and systematic uncertainties, respectively.
description: Two-particle transverse momentum differential correlators, recently measured in Pb$-$Pb collisions at LHC energies, provide an additional tool to gain insights into particle production mechanisms and infer transport properties, such as the ratio of shear viscosity to entropy density, of the medium created in Pb$-$Pb collisions. The longitudinal long-range correlations and the large azimuthal anisotropy measured at low transverse momenta in small collision systems, namely pp and p$-$Pb, at LHC energies resemble manifestations of collective behaviour. This suggests that locally equilibrated matter may be produced in these small collision systems, similar to what is observed in Pb$-$Pb collisions. In this work, the same two-particle transverse momentum differential correlators are exploited in pp and p$-$Pb collisions at $\sqrt{s} = 7\;\text{TeV}$ and $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$, respectively, to seek evidence for viscous effects. Specifically, the strength and shape of the correlators are studied as a function of the produced particle multiplicity to identify evidence for longitudinal broadening that might reveal the presence of viscous effects in these smaller systems. The measured correlators and their evolution from pp and p$-$Pb to Pb$-$Pb collisions are additionally compared to predictions from Monte Carlo event generators, and the potential presence of viscous effects is discussed.
DOI: 10.17182/hepdata.146027.v1/t5
title: "Figure 2b bottom" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Fragmentation modification ratios for charged jets for low pT for the different toy modifications.
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t6
title: "Figure 3a top R020" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet production spectra in 0--10% collisions with R = 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t7
title: "Figure 3a top R040" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet production spectra in 0--10% collisions with R = 0.4
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t8
title: "Figure 3a top R060" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet production spectra in 0--10% collisions with R = 0.6
description: No data abstract available.
DOI: 10.17182/hepdata.137819.v1/t24
title: "Figure 5.4" of "Two-particle transverse momentum correlations in pp and p-Pb collisions at LHC energies"

description: Evolution with the average charged particle multiplicity of the azimuthal widths of the two-particle transverse momentum differential correlation $G_{2}^{\rm CI}$ in pp and p$-$Pb collisions at $\sqrt{s} = 7\;\text{TeV}$ and $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$, respectively. Vertical bars (mostly smaller than the marker size) and filled boxes represent statistical and systematic uncertainties, respectively.
description: Two-particle transverse momentum differential correlators, recently measured in Pb$-$Pb collisions at LHC energies, provide an additional tool to gain insights into particle production mechanisms and infer transport properties, such as the ratio of shear viscosity to entropy density, of the medium created in Pb$-$Pb collisions. The longitudinal long-range correlations and the large azimuthal anisotropy measured at low transverse momenta in small collision systems, namely pp and p$-$Pb, at LHC energies resemble manifestations of collective behaviour. This suggests that locally equilibrated matter may be produced in these small collision systems, similar to what is observed in Pb$-$Pb collisions. In this work, the same two-particle transverse momentum differential correlators are exploited in pp and p$-$Pb collisions at $\sqrt{s} = 7\;\text{TeV}$ and $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$, respectively, to seek evidence for viscous effects. Specifically, the strength and shape of the correlators are studied as a function of the produced particle multiplicity to identify evidence for longitudinal broadening that might reveal the presence of viscous effects in these smaller systems. The measured correlators and their evolution from pp and p$-$Pb to Pb$-$Pb collisions are additionally compared to predictions from Monte Carlo event generators, and the potential presence of viscous effects is discussed.
DOI: 10.17182/hepdata.146027.v1/t10
title: "Figure 3b top R040" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet production spectra in 30--50% collisions with R = 0.4
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t11
title: "Figure 3b top R060" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet production spectra in 30--50% collisions with R = 0.6
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t12
title: "Figure 3a bottom" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet production spectra in 60--80% collisions
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t13
title: "Figure 3b bottom" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet production spectra in pp collisions
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t14
title: "Figure 4a top ML" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.2 in central collisions with ML-based subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t16
title: "Figure 4b top AB" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.4 in central collisions with AB subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t9
title: "Figure 3b top R020" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet production spectra in 30--50% collisions with R = 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.132766.v1/t1
title: "Table 1" of "Constraining the ${\rm\overline{K}N}$ coupled channel dynamics using femtoscopic correlations at the LHC"

description: K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in pp collisions at $\sqrt{s}=13$ TeV.
description: The interaction of K$^-$ with protons is characterised by the presence of several coupled channels, systems like $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ with a similar mass and the same quantum numbers as the K$^-$p state. The strengths of these couplings to the K$^-$p system are of crucial importance for the understanding of the nature of the $\Lambda(1405)$ resonance and of the attractive K$^-$p strong interaction. In this article, we present measurements of the K$^-$p correlation functions in relative momentum space obtained in pp collisions at $\sqrt{s}$ = 13 TeV, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV, and (semi)peripheral Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The emitting source size, composed of a core radius anchored to the K$^+$p correlation and of a resonance halo specific to each particle pair, varies between 1 and 2 fm in these collision systems. The strength and the effects of the $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ inelastic channels on the measured K$^-$p correlation function are investigated in the different colliding systems by comparing the data with state-of-the-art models of chiral potentials. A novel approach to determine the conversion weights $\omega$, necessary to quantify the amount of produced inelastic channels in the correlation function, is presented. In this method, particle yields are estimated from thermal model predictions, and their kinematic distribution from blast-wave fits to measured data. The comparison of chiral potentials to the measured K$^-$p interaction indicates that, while the $\pi \Sigma$-K$^-$p dynamics is well reproduced by the model, the coupling to the $\mathrm{\overline{K}^0 n}$ channel in the model is currently underestimated.
DOI: 10.17182/hepdata.146027.v1/t15
title: "Figure 4a top AB" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.2 in central collisions with AB subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t17
title: "Figure 4b top ML" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.4 in central collisions with ML subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t18
title: "Figure 4c top ML" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.6 in central collisions with ML subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t19
title: "Figure 4a middle ML" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.2 in semicentral collisions with ML-based subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t20
title: "Figure 4a middle AB" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.2 in semicentral collisions with AB subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t21
title: "Figure 4b middle ML" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.4 in semicentral collisions with ML-based subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t22
title: "Figure 4b middle AB" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.4 in semicentral collisions with AB subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t23
title: "Figure 4c middle AB" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.6 in semicentral collisions with AB subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.132766.v1/t2
title: "Table 2a" of "Constraining the ${\rm\overline{K}N}$ coupled channel dynamics using femtoscopic correlations at the LHC"

description: K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in p-Pb collisions at $\sqrt{s_{\mathrm {NN}}}=5.02 $ TeV (0-20%).
description: The interaction of K$^-$ with protons is characterised by the presence of several coupled channels, systems like $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ with a similar mass and the same quantum numbers as the K$^-$p state. The strengths of these couplings to the K$^-$p system are of crucial importance for the understanding of the nature of the $\Lambda(1405)$ resonance and of the attractive K$^-$p strong interaction. In this article, we present measurements of the K$^-$p correlation functions in relative momentum space obtained in pp collisions at $\sqrt{s}$ = 13 TeV, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV, and (semi)peripheral Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The emitting source size, composed of a core radius anchored to the K$^+$p correlation and of a resonance halo specific to each particle pair, varies between 1 and 2 fm in these collision systems. The strength and the effects of the $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ inelastic channels on the measured K$^-$p correlation function are investigated in the different colliding systems by comparing the data with state-of-the-art models of chiral potentials. A novel approach to determine the conversion weights $\omega$, necessary to quantify the amount of produced inelastic channels in the correlation function, is presented. In this method, particle yields are estimated from thermal model predictions, and their kinematic distribution from blast-wave fits to measured data. The comparison of chiral potentials to the measured K$^-$p interaction indicates that, while the $\pi \Sigma$-K$^-$p dynamics is well reproduced by the model, the coupling to the $\mathrm{\overline{K}^0 n}$ channel in the model is currently underestimated.
DOI: 10.17182/hepdata.132766.v1/t3
title: "Table 2b" of "Constraining the ${\rm\overline{K}N}$ coupled channel dynamics using femtoscopic correlations at the LHC"

description: K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV (20-40%).
description: The interaction of K$^-$ with protons is characterised by the presence of several coupled channels, systems like $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ with a similar mass and the same quantum numbers as the K$^-$p state. The strengths of these couplings to the K$^-$p system are of crucial importance for the understanding of the nature of the $\Lambda(1405)$ resonance and of the attractive K$^-$p strong interaction. In this article, we present measurements of the K$^-$p correlation functions in relative momentum space obtained in pp collisions at $\sqrt{s}$ = 13 TeV, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV, and (semi)peripheral Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The emitting source size, composed of a core radius anchored to the K$^+$p correlation and of a resonance halo specific to each particle pair, varies between 1 and 2 fm in these collision systems. The strength and the effects of the $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ inelastic channels on the measured K$^-$p correlation function are investigated in the different colliding systems by comparing the data with state-of-the-art models of chiral potentials. A novel approach to determine the conversion weights $\omega$, necessary to quantify the amount of produced inelastic channels in the correlation function, is presented. In this method, particle yields are estimated from thermal model predictions, and their kinematic distribution from blast-wave fits to measured data. The comparison of chiral potentials to the measured K$^-$p interaction indicates that, while the $\pi \Sigma$-K$^-$p dynamics is well reproduced by the model, the coupling to the $\mathrm{\overline{K}^0 n}$ channel in the model is currently underestimated.
DOI: 10.17182/hepdata.132766.v1/t4
title: "Table 2c" of "Constraining the ${\rm\overline{K}N}$ coupled channel dynamics using femtoscopic correlations at the LHC"

description: K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (40-100%).
description: The interaction of K$^-$ with protons is characterised by the presence of several coupled channels, systems like $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ with a similar mass and the same quantum numbers as the K$^-$p state. The strengths of these couplings to the K$^-$p system are of crucial importance for the understanding of the nature of the $\Lambda(1405)$ resonance and of the attractive K$^-$p strong interaction. In this article, we present measurements of the K$^-$p correlation functions in relative momentum space obtained in pp collisions at $\sqrt{s}$ = 13 TeV, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV, and (semi)peripheral Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The emitting source size, composed of a core radius anchored to the K$^+$p correlation and of a resonance halo specific to each particle pair, varies between 1 and 2 fm in these collision systems. The strength and the effects of the $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ inelastic channels on the measured K$^-$p correlation function are investigated in the different colliding systems by comparing the data with state-of-the-art models of chiral potentials. A novel approach to determine the conversion weights $\omega$, necessary to quantify the amount of produced inelastic channels in the correlation function, is presented. In this method, particle yields are estimated from thermal model predictions, and their kinematic distribution from blast-wave fits to measured data. The comparison of chiral potentials to the measured K$^-$p interaction indicates that, while the $\pi \Sigma$-K$^-$p dynamics is well reproduced by the model, the coupling to the $\mathrm{\overline{K}^0 n}$ channel in the model is currently underestimated.
DOI: 10.17182/hepdata.146027.v1/t24
title: "Figure 4a bottom AB" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.2 in peripheral collisions with AB subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t25
title: "Figure 4b bottom AB" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor for jets with R = 0.4 in peripheral collisions with AB subtraction
description: No data abstract available.
DOI: 10.17182/hepdata.146027.v1/t27
title: "Figure 7a pp" of "Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Cross Section ratios for pp
description: No data abstract available.
DOI: 10.17182/hepdata.132766.v1/t5
title: "Table 3a" of "Constraining the ${\rm\overline{K}N}$ coupled channel dynamics using femtoscopic correlations at the LHC"

description: K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (60-70%).
description: The interaction of K$^-$ with protons is characterised by the presence of several coupled channels, systems like $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ with a similar mass and the same quantum numbers as the K$^-$p state. The strengths of these couplings to the K$^-$p system are of crucial importance for the understanding of the nature of the $\Lambda(1405)$ resonance and of the attractive K$^-$p strong interaction. In this article, we present measurements of the K$^-$p correlation functions in relative momentum space obtained in pp collisions at $\sqrt{s}$ = 13 TeV, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV, and (semi)peripheral Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The emitting source size, composed of a core radius anchored to the K$^+$p correlation and of a resonance halo specific to each particle pair, varies between 1 and 2 fm in these collision systems. The strength and the effects of the $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ inelastic channels on the measured K$^-$p correlation function are investigated in the different colliding systems by comparing the data with state-of-the-art models of chiral potentials. A novel approach to determine the conversion weights $\omega$, necessary to quantify the amount of produced inelastic channels in the correlation function, is presented. In this method, particle yields are estimated from thermal model predictions, and their kinematic distribution from blast-wave fits to measured data. The comparison of chiral potentials to the measured K$^-$p interaction indicates that, while the $\pi \Sigma$-K$^-$p dynamics is well reproduced by the model, the coupling to the $\mathrm{\overline{K}^0 n}$ channel in the model is currently underestimated.