cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83664.v1/t1
title: "Table 1" of "Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV"

description: The measured values of the angular parameters and the $\Lambda_b$ polarization.
description: An analysis of the bottom baryon decay $\Lambda_{b}\to J/\psi \Lambda$ is performed to measure the $\Lambda_b$ polarization and three angular parameters in data from pp collisions at $\sqrt{s} = 7$ and $8\, {\rm TeV}$, collected by the CMS experiment at the Large Hadron Collider. The $\Lambda_b$ polarization is measured to be $0.00\pm0.06$ (stat) $\pm0.06$ (syst) and the parity-violating asymmetry parameter is determined to be $-0.14\pm0.14$ (stat) $\pm0.10$ (syst). The measurements are compared to various theoretical predictions, including those from perturbative quantum chromodynamics.
DOI: 10.17182/hepdata.83664.v1/t2
title: "Table 2" of "Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV"

description: The values of the helicity amplitudes in the decay.
description: An analysis of the bottom baryon decay $\Lambda_{b}\to J/\psi \Lambda$ is performed to measure the $\Lambda_b$ polarization and three angular parameters in data from pp collisions at $\sqrt{s} = 7$ and $8\, {\rm TeV}$, collected by the CMS experiment at the Large Hadron Collider. The $\Lambda_b$ polarization is measured to be $0.00\pm0.06$ (stat) $\pm0.06$ (syst) and the parity-violating asymmetry parameter is determined to be $-0.14\pm0.14$ (stat) $\pm0.10$ (syst). The measurements are compared to various theoretical predictions, including those from perturbative quantum chromodynamics.
DOI: 10.17182/hepdata.83664.v1/t3
title: "Table 3" of "Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV"

description: Correlation matrix for the fitted parameters.
description: An analysis of the bottom baryon decay $\Lambda_{b}\to J/\psi \Lambda$ is performed to measure the $\Lambda_b$ polarization and three angular parameters in data from pp collisions at $\sqrt{s} = 7$ and $8\, {\rm TeV}$, collected by the CMS experiment at the Large Hadron Collider. The $\Lambda_b$ polarization is measured to be $0.00\pm0.06$ (stat) $\pm0.06$ (syst) and the parity-violating asymmetry parameter is determined to be $-0.14\pm0.14$ (stat) $\pm0.10$ (syst). The measurements are compared to various theoretical predictions, including those from perturbative quantum chromodynamics.
DOI: 10.17182/hepdata.83685.v1/t1
title: "Table 1" of "Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Best fit values in the signal strength modifiers (mu), and their 68% CL intervals as split into the statistical and systematic components for each category and combinations of categories.
description: Search for ttH production in the all-jet final state in proton-proton collisions at sqrt(s) = 13 TeV.

No cross section measurements are performed. Data reported here are signal strengths relative to the standard model prediction and data extracted from the signal-to-background plot (logS/B). All information presented in the paper JHEP 06 (2018) 10.
DOI: 10.17182/hepdata.83685.v1/t2
title: "Table 2" of "Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Values of log10(S/B), where S and B indicate the respective bin-by-bin yields of the signal and background expected in the MEM discriminant distributions, obtained from a combined fit with the constraint in the cross section of mu = 1.
description: Search for ttH production in the all-jet final state in proton-proton collisions at sqrt(s) = 13 TeV.

No cross section measurements are performed. Data reported here are signal strengths relative to the standard model prediction and data extracted from the signal-to-background plot (logS/B). All information presented in the paper JHEP 06 (2018) 10.
DOI: 10.17182/hepdata.83700.v1/t1
title: "Table 1" of "Neutral pion and $\eta$ meson production in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}} = 5.02$ TeV"

description: Invariant differential yield of PI0 produced in NSD p-Pp collisions with centre-of-mass energy/nucleon 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.83700.v1/t2
title: "Table 2" of "Neutral pion and $\eta$ meson production in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}} = 5.02$ TeV"

description: Invariant differential yields of ETA produced in NSD p-Pb collisions with centre-of-mass energy/nucleon 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.83700.v1/t3
title: "Table 3" of "Neutral pion and $\eta$ meson production in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}} = 5.02$ TeV"

description: The measured ratio of invariant yields for inclusive ETA to PI0 production at a centre-of-mass energy/nucleon 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.83700.v1/t4
title: "Table 4" of "Neutral pion and $\eta$ meson production in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}} = 5.02$ TeV"

description: Ratio of the measured ETA to PI0 ratio to the one obtained via m_T scaling in NSD p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.83700.v1/t5
title: "Table 5" of "Neutral pion and $\eta$ meson production in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}} = 5.02$ TeV"

description: The nuclear modification factor RPPB of PI0 as a function of pT in NSD p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, the overall normalization uncertainty of 5.96 % is not included.
description: No data abstract available.
DOI: 10.17182/hepdata.83700.v1/t6
title: "Table 6" of "Neutral pion and $\eta$ meson production in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}} = 5.02$ TeV"

description: The nuclear modification factor RPPB of ETA as a function of pT in NSD p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, the overall normalization uncertainty of 5.96 % is not included.
description: No data abstract available.
DOI: 10.17182/hepdata.83702.v1/t1
title: "Table 1" of "Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: The y-differential inclusive JPsi cross section obtained in p-Pb and Pb-p collisions. 
The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third one is the global uncertainty common to p-Pb and Pb-p results.
description: CERN-LHC. Inclusive J/Psi production is studied in pPb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) =8.16 TeV, using the ALICE detector at the CERN LHC. The J/Psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03
DOI: 10.17182/hepdata.83702.v1/t2
title: "Table 2" of "Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: The pt-differential inclusive JPsi cross section obtained in Pb-p collisions. 
The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third one is the global uncertainty common to p-Pb and Pb-p results.
description: CERN-LHC. Inclusive J/Psi production is studied in pPb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) =8.16 TeV, using the ALICE detector at the CERN LHC. The J/Psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03
DOI: 10.17182/hepdata.83702.v1/t3
title: "Table 3" of "Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: The pt-differential inclusive JPsi nuclear modification factor obtained in p-Pb. 
The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third one is the global uncertainty common to p-Pb and Pb-p results.
description: CERN-LHC. Inclusive J/Psi production is studied in pPb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) =8.16 TeV, using the ALICE detector at the CERN LHC. The J/Psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03
DOI: 10.17182/hepdata.83702.v1/t4
title: "Table 4" of "Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: The rapidity dependence of the inclusive JPsi nuclear modification factor obtained in p-Pb and Pb-p collisions. The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third is a global uncertainty common to p-Pb and Pb-p results.
description: CERN-LHC. Inclusive J/Psi production is studied in pPb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) =8.16 TeV, using the ALICE detector at the CERN LHC. The J/Psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03
DOI: 10.17182/hepdata.83702.v1/t5
title: "Table 5" of "Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: The pt-differential inclusive JPsi nuclear modification factor obtained in Pb-p collisions. 
The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third one is the global uncertainty common to all the pT values.
description: CERN-LHC. Inclusive J/Psi production is studied in pPb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) =8.16 TeV, using the ALICE detector at the CERN LHC. The J/Psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03
DOI: 10.17182/hepdata.83702.v1/t7
title: "Table 7" of "Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: The forward to backward ratio RFB of the inclusive JPsi nuclear modification factors. 
The first uncertainty is statistical, the second one is systematic.
description: CERN-LHC. Inclusive J/Psi production is studied in pPb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) =8.16 TeV, using the ALICE detector at the CERN LHC. The J/Psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03
DOI: 10.17182/hepdata.83702.v1/t6
title: "Table 6" of "Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: The pt-differential inclusive JPsi nuclear modification factor obtained in p-Pb collisions. 
The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third one is the global uncertainty common to all the pT values.
description: CERN-LHC. Inclusive J/Psi production is studied in pPb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) =8.16 TeV, using the ALICE detector at the CERN LHC. The J/Psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03
DOI: 10.17182/hepdata.83702.v1/t8
title: "Table 8" of "Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: The pT dependence of the forward to backward ratio RFB of the inclusive JPsi nuclear modification factors. 
The first uncertainty is statistical, while the second is the systematic uncertainty.
description: CERN-LHC. Inclusive J/Psi production is studied in pPb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) =8.16 TeV, using the ALICE detector at the CERN LHC. The J/Psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03
DOI: 10.17182/hepdata.83737.v1/t1
title: "Table 1" of "Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_\text{NN}}} = \mathbf{5.02}$ and $\mathbf{2.76}$ TeV"

description: $v_2\{2,|\Delta\eta| &gt; 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: Measurements of anisotropic flow coefficients with two- and multi-particle cumulants for inclusive charged particles in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV are reported in the pseudorapidity range $|\eta| &lt; 0.8$ and transverse momentum $0.2 &lt; p_\text{T} &lt; 50$ GeV/$c$. The full data sample collected by the ALICE detector in 2015 (2010), corresponding to an integrated luminosity of 12.7 (2.0) $\mu$b$^{-1}$ in the centrality range 0-80$\%$, is analysed. Flow coefficients up to the sixth flow harmonic ($v_6$) are reported and a detailed comparison among results at the two energies is carried out. The $p_\text{T}$ dependence of anisotropic flow coefficients and its evolution with respect to centrality and harmonic number $n$ are investigated. An approximate power-law scaling of the form $v_n(p_\text{T}) \sim p_\text{T}^{n/3}$ is observed for all flow harmonics at low $p_\text{T}$ ($0.2 &lt; p_\text{T} &lt; 3$ GeV/$c$). At the same time, the ratios $v_n/v_m^{n/m}$ are observed to be essentially independent of $p_\text{T}$ for most centralities up to about $p_\text{T} = 10$ GeV/$c$. Analysing the differences among higher-order cumulants of elliptic flow ($v_2$), which have different sensitivities to flow fluctuations, a measurement of the standardised skewness of the event-by-event $v_2$ distribution $P(v_2)$ is reported and constraints on its higher moments are provided. The Elliptic Power distribution is used to parametrise $P(v_2)$, extracting its parameters from fits to cumulants. The measurements are compared to different model predictions in order to discriminate among initial-state models and to constrain the temperature dependence of the shear viscosity to entropy-density ratio.
DOI: 10.17182/hepdata.83737.v1/t2
title: "Table 2" of "Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_\text{NN}}} = \mathbf{5.02}$ and $\mathbf{2.76}$ TeV"

description: $v_2\{4\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: Measurements of anisotropic flow coefficients with two- and multi-particle cumulants for inclusive charged particles in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV are reported in the pseudorapidity range $|\eta| &lt; 0.8$ and transverse momentum $0.2 &lt; p_\text{T} &lt; 50$ GeV/$c$. The full data sample collected by the ALICE detector in 2015 (2010), corresponding to an integrated luminosity of 12.7 (2.0) $\mu$b$^{-1}$ in the centrality range 0-80$\%$, is analysed. Flow coefficients up to the sixth flow harmonic ($v_6$) are reported and a detailed comparison among results at the two energies is carried out. The $p_\text{T}$ dependence of anisotropic flow coefficients and its evolution with respect to centrality and harmonic number $n$ are investigated. An approximate power-law scaling of the form $v_n(p_\text{T}) \sim p_\text{T}^{n/3}$ is observed for all flow harmonics at low $p_\text{T}$ ($0.2 &lt; p_\text{T} &lt; 3$ GeV/$c$). At the same time, the ratios $v_n/v_m^{n/m}$ are observed to be essentially independent of $p_\text{T}$ for most centralities up to about $p_\text{T} = 10$ GeV/$c$. Analysing the differences among higher-order cumulants of elliptic flow ($v_2$), which have different sensitivities to flow fluctuations, a measurement of the standardised skewness of the event-by-event $v_2$ distribution $P(v_2)$ is reported and constraints on its higher moments are provided. The Elliptic Power distribution is used to parametrise $P(v_2)$, extracting its parameters from fits to cumulants. The measurements are compared to different model predictions in order to discriminate among initial-state models and to constrain the temperature dependence of the shear viscosity to entropy-density ratio.
DOI: 10.17182/hepdata.83737.v1/t3
title: "Table 3" of "Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_\text{NN}}} = \mathbf{5.02}$ and $\mathbf{2.76}$ TeV"

description: $v_3\{2,|\Delta\eta| &gt; 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: Measurements of anisotropic flow coefficients with two- and multi-particle cumulants for inclusive charged particles in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV are reported in the pseudorapidity range $|\eta| &lt; 0.8$ and transverse momentum $0.2 &lt; p_\text{T} &lt; 50$ GeV/$c$. The full data sample collected by the ALICE detector in 2015 (2010), corresponding to an integrated luminosity of 12.7 (2.0) $\mu$b$^{-1}$ in the centrality range 0-80$\%$, is analysed. Flow coefficients up to the sixth flow harmonic ($v_6$) are reported and a detailed comparison among results at the two energies is carried out. The $p_\text{T}$ dependence of anisotropic flow coefficients and its evolution with respect to centrality and harmonic number $n$ are investigated. An approximate power-law scaling of the form $v_n(p_\text{T}) \sim p_\text{T}^{n/3}$ is observed for all flow harmonics at low $p_\text{T}$ ($0.2 &lt; p_\text{T} &lt; 3$ GeV/$c$). At the same time, the ratios $v_n/v_m^{n/m}$ are observed to be essentially independent of $p_\text{T}$ for most centralities up to about $p_\text{T} = 10$ GeV/$c$. Analysing the differences among higher-order cumulants of elliptic flow ($v_2$), which have different sensitivities to flow fluctuations, a measurement of the standardised skewness of the event-by-event $v_2$ distribution $P(v_2)$ is reported and constraints on its higher moments are provided. The Elliptic Power distribution is used to parametrise $P(v_2)$, extracting its parameters from fits to cumulants. The measurements are compared to different model predictions in order to discriminate among initial-state models and to constrain the temperature dependence of the shear viscosity to entropy-density ratio.
DOI: 10.17182/hepdata.83737.v1/t4
title: "Table 4" of "Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_\text{NN}}} = \mathbf{5.02}$ and $\mathbf{2.76}$ TeV"

description: $v_4\{2,|\Delta\eta| &gt; 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: Measurements of anisotropic flow coefficients with two- and multi-particle cumulants for inclusive charged particles in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV are reported in the pseudorapidity range $|\eta| &lt; 0.8$ and transverse momentum $0.2 &lt; p_\text{T} &lt; 50$ GeV/$c$. The full data sample collected by the ALICE detector in 2015 (2010), corresponding to an integrated luminosity of 12.7 (2.0) $\mu$b$^{-1}$ in the centrality range 0-80$\%$, is analysed. Flow coefficients up to the sixth flow harmonic ($v_6$) are reported and a detailed comparison among results at the two energies is carried out. The $p_\text{T}$ dependence of anisotropic flow coefficients and its evolution with respect to centrality and harmonic number $n$ are investigated. An approximate power-law scaling of the form $v_n(p_\text{T}) \sim p_\text{T}^{n/3}$ is observed for all flow harmonics at low $p_\text{T}$ ($0.2 &lt; p_\text{T} &lt; 3$ GeV/$c$). At the same time, the ratios $v_n/v_m^{n/m}$ are observed to be essentially independent of $p_\text{T}$ for most centralities up to about $p_\text{T} = 10$ GeV/$c$. Analysing the differences among higher-order cumulants of elliptic flow ($v_2$), which have different sensitivities to flow fluctuations, a measurement of the standardised skewness of the event-by-event $v_2$ distribution $P(v_2)$ is reported and constraints on its higher moments are provided. The Elliptic Power distribution is used to parametrise $P(v_2)$, extracting its parameters from fits to cumulants. The measurements are compared to different model predictions in order to discriminate among initial-state models and to constrain the temperature dependence of the shear viscosity to entropy-density ratio.
DOI: 10.17182/hepdata.83737.v1/t5
title: "Table 5" of "Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_\text{NN}}} = \mathbf{5.02}$ and $\mathbf{2.76}$ TeV"

description: $v_5\{2,|\Delta\eta| &gt; 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: Measurements of anisotropic flow coefficients with two- and multi-particle cumulants for inclusive charged particles in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV are reported in the pseudorapidity range $|\eta| &lt; 0.8$ and transverse momentum $0.2 &lt; p_\text{T} &lt; 50$ GeV/$c$. The full data sample collected by the ALICE detector in 2015 (2010), corresponding to an integrated luminosity of 12.7 (2.0) $\mu$b$^{-1}$ in the centrality range 0-80$\%$, is analysed. Flow coefficients up to the sixth flow harmonic ($v_6$) are reported and a detailed comparison among results at the two energies is carried out. The $p_\text{T}$ dependence of anisotropic flow coefficients and its evolution with respect to centrality and harmonic number $n$ are investigated. An approximate power-law scaling of the form $v_n(p_\text{T}) \sim p_\text{T}^{n/3}$ is observed for all flow harmonics at low $p_\text{T}$ ($0.2 &lt; p_\text{T} &lt; 3$ GeV/$c$). At the same time, the ratios $v_n/v_m^{n/m}$ are observed to be essentially independent of $p_\text{T}$ for most centralities up to about $p_\text{T} = 10$ GeV/$c$. Analysing the differences among higher-order cumulants of elliptic flow ($v_2$), which have different sensitivities to flow fluctuations, a measurement of the standardised skewness of the event-by-event $v_2$ distribution $P(v_2)$ is reported and constraints on its higher moments are provided. The Elliptic Power distribution is used to parametrise $P(v_2)$, extracting its parameters from fits to cumulants. The measurements are compared to different model predictions in order to discriminate among initial-state models and to constrain the temperature dependence of the shear viscosity to entropy-density ratio.