cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.105915.v1/t43
title: "Figure 4 (a)" of "Beam energy dependence of moments of the net-charge multiplicity distributions in Au+Au collisions at RHIC"

description: The efficiency and centrality bin width corrected $\sigma^2/M$ of the net-charge multiplicity distributions as a function of collision energy for Au+Au collisions. The error bars are statistical and the caps represent systematic errors.
description: We report the first measurements of the moments - mean ($M$), variance ($\sigma^{2}$), skewness ($S$) and kurtosis ($\kappa$) - of the net-charge multiplicity distributions at mid-rapidity in Au+Au collisions at seven energies, ranging from $\sqrt{s_{NN}}=$ 7.7 to 200~GeV, as a part of the Beam Energy Scan program at RHIC. The moments are related to the thermodynamic susceptibilities of net-charge, and are sensitive to the location of the QCD critical point. We compare the products of the moments, $\sigma^{2}/M$, $S\sigma$ and $\kappa\sigma^{2}$ with the expectations from Poisson and negative binomial distributions (NBD). The $S\sigma$ values deviate from Poisson and are close to NBD baseline, while the $\kappa\sigma^{2}$ values tend to lie between the two. Within the present uncertainties, our data do not show non-monotonic behavior as a function of collision energy. These measurements provide a valuable tool to extract the freeze-out parameters in heavy-ion collisions by comparing with theoretical models.
DOI: 10.17182/hepdata.105915.v1/t44
title: "Figure 4 (b)" of "Beam energy dependence of moments of the net-charge multiplicity distributions in Au+Au collisions at RHIC"

description: The efficiency and centrality bin width corrected $S\sigma^2$ of the net-charge multiplicity distributions as a function of collision energy for Au+Au collisions. The error bars are statistical and the caps represent systematic errors.
description: We report the first measurements of the moments - mean ($M$), variance ($\sigma^{2}$), skewness ($S$) and kurtosis ($\kappa$) - of the net-charge multiplicity distributions at mid-rapidity in Au+Au collisions at seven energies, ranging from $\sqrt{s_{NN}}=$ 7.7 to 200~GeV, as a part of the Beam Energy Scan program at RHIC. The moments are related to the thermodynamic susceptibilities of net-charge, and are sensitive to the location of the QCD critical point. We compare the products of the moments, $\sigma^{2}/M$, $S\sigma$ and $\kappa\sigma^{2}$ with the expectations from Poisson and negative binomial distributions (NBD). The $S\sigma$ values deviate from Poisson and are close to NBD baseline, while the $\kappa\sigma^{2}$ values tend to lie between the two. Within the present uncertainties, our data do not show non-monotonic behavior as a function of collision energy. These measurements provide a valuable tool to extract the freeze-out parameters in heavy-ion collisions by comparing with theoretical models.
DOI: 10.17182/hepdata.105915.v1/t45
title: "Figure 4 (c)" of "Beam energy dependence of moments of the net-charge multiplicity distributions in Au+Au collisions at RHIC"

description: The efficiency and centrality bin width corrected $\kappa\sigma^2$ of the net-charge multiplicity distributions as a function of collision energy for Au+Au collisions. The error bars are statistical and the caps represent systematic errors.
description: We report the first measurements of the moments - mean ($M$), variance ($\sigma^{2}$), skewness ($S$) and kurtosis ($\kappa$) - of the net-charge multiplicity distributions at mid-rapidity in Au+Au collisions at seven energies, ranging from $\sqrt{s_{NN}}=$ 7.7 to 200~GeV, as a part of the Beam Energy Scan program at RHIC. The moments are related to the thermodynamic susceptibilities of net-charge, and are sensitive to the location of the QCD critical point. We compare the products of the moments, $\sigma^{2}/M$, $S\sigma$ and $\kappa\sigma^{2}$ with the expectations from Poisson and negative binomial distributions (NBD). The $S\sigma$ values deviate from Poisson and are close to NBD baseline, while the $\kappa\sigma^{2}$ values tend to lie between the two. Within the present uncertainties, our data do not show non-monotonic behavior as a function of collision energy. These measurements provide a valuable tool to extract the freeze-out parameters in heavy-ion collisions by comparing with theoretical models.
DOI: 10.17182/hepdata.105961.v1/t1
title: "Table 1" of "Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\tau$ leptons in pp collisions at $\sqrt{s} = $ 13 TeV"

description: The fiducial differential signal strength and cross section in each Higgs pT bin. Both the unregularized and regularized signal strengths are given; they do not include uncertainties in the SM signal normalization. The fiducial cross section and its full uncertainty in each bin are also given. The last bin is inclusive.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; TAU + TAU - decay mode. The measurements are performed using data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the visible tau decay products and missing pT. The jets are defined in accordance with STXS jet definition. The differential cross section times branching fraction is measured as a function of the Higgs boson pT, jet multiplicity, and pT of the leading jet, in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. Results are unfolded to particle level.
DOI: 10.17182/hepdata.105961.v1/t2
title: "Table 2" of "Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\tau$ leptons in pp collisions at $\sqrt{s} = $ 13 TeV"

description: The fiducial differential signal strength and cross section in each jet multiplicity bin. Both the unregularized and regularized signal strengths are given; they do not include uncertainties in the SM signal normalization. The fiducial cross section and its full uncertainty in each bin are also given. The last bin is inclusive.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; TAU + TAU - decay mode. The measurements are performed using data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the visible tau decay products and missing pT. The jets are defined in accordance with STXS jet definition. The differential cross section times branching fraction is measured as a function of the Higgs boson pT, jet multiplicity, and pT of the leading jet, in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. Results are unfolded to particle level.
DOI: 10.17182/hepdata.105961.v1/t3
title: "Table 3" of "Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\tau$ leptons in pp collisions at $\sqrt{s} = $ 13 TeV"

description: The fiducial differential signal strength and cross section in each leading jet pT bin. Both the unregularized and regularized signal strengths are given; they do not include uncertainties in the SM signal normalization. The fiducial cross section and its full uncertainty in each bin are also given. The last bin is inclusive.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; TAU + TAU - decay mode. The measurements are performed using data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the visible tau decay products and missing pT. The jets are defined in accordance with STXS jet definition. The differential cross section times branching fraction is measured as a function of the Higgs boson pT, jet multiplicity, and pT of the leading jet, in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. Results are unfolded to particle level.
DOI: 10.17182/hepdata.105961.v1/t4
title: "Table 4" of "Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\tau$ leptons in pp collisions at $\sqrt{s} = $ 13 TeV"

description: The correlation matrix for the Higgs pT measurements, both for the unregularized and regularized fits. The last bin is inclusive.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; TAU + TAU - decay mode. The measurements are performed using data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the visible tau decay products and missing pT. The jets are defined in accordance with STXS jet definition. The differential cross section times branching fraction is measured as a function of the Higgs boson pT, jet multiplicity, and pT of the leading jet, in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. Results are unfolded to particle level.
DOI: 10.17182/hepdata.105961.v1/t5
title: "Table 5" of "Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\tau$ leptons in pp collisions at $\sqrt{s} = $ 13 TeV"

description: The correlation matrix for the jet multiplicity measurements, both for the unregularized and regularized fits. The last bin is inclusive.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; TAU + TAU - decay mode. The measurements are performed using data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the visible tau decay products and missing pT. The jets are defined in accordance with STXS jet definition. The differential cross section times branching fraction is measured as a function of the Higgs boson pT, jet multiplicity, and pT of the leading jet, in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. Results are unfolded to particle level.
DOI: 10.17182/hepdata.105961.v1/t6
title: "Table 6" of "Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\tau$ leptons in pp collisions at $\sqrt{s} = $ 13 TeV"

description: The correlation matrix for the leading jet pT measurements, both for the unregularized and regularized fits. The last bin is inclusive.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; TAU + TAU - decay mode. The measurements are performed using data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the visible tau decay products and missing pT. The jets are defined in accordance with STXS jet definition. The differential cross section times branching fraction is measured as a function of the Higgs boson pT, jet multiplicity, and pT of the leading jet, in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. Results are unfolded to particle level.
DOI: 10.17182/hepdata.105961.v1/t7
title: "Table 7" of "Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\tau$ leptons in pp collisions at $\sqrt{s} = $ 13 TeV"

description: The fiducial integrated signal strength and cross section.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; TAU + TAU - decay mode. The measurements are performed using data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the visible tau decay products and missing pT. The jets are defined in accordance with STXS jet definition. The differential cross section times branching fraction is measured as a function of the Higgs boson pT, jet multiplicity, and pT of the leading jet, in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. Results are unfolded to particle level.
DOI: 10.25549/vercoutere-ouc110611140
title: Portrait of a man wearing a brimless cap

description: Portrait of a male with white hair and beard, blue eyes wearing a black brimless cap (kufi or kippa?), and a robe with yellow, white, pink, and gray strips; brown, tan, and red background
DOI: 10.17182/hepdata.105975.v1/t1
title: "Table 1" of "Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV"

description: The per-trigger associated yield versus $\Delta\varphi$ for charged particles with $p_{\rm T}&gt;5.0$ GeV/$c$ and associate deuterons and anti-deuterons for 1.0-1.35 GeV/$c$.
description: CERN-LHC. Deuteron production in high-energy collisions is sensitive to the space-time evolution of the collision system, and is typically described by a coalescence mechanism. For the first time, we present results on jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV, providing an opportunity to test the established picture for deuteron production in events with a hard scattering. Using a trigger particle with high transverse-momentum~($p_{\rm T}&gt;5$ GeV/$c$) as a proxy for the presence of a jet at mid-rapidity, we observe a measurable population of deuterons being produced around the jet proxy. The associated deuteron yield measured in a narrow angular range around the trigger particle differs by 2--3 standard deviations from the uncorrelated background. The data are described by PYTHIA model calculations featuring baryon coalescence.
DOI: 10.17182/hepdata.105975.v1/t2
title: "Table 2" of "Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV"

description: The per-trigger associated yield versus $\Delta\varphi$ for charged particles with $p_{\rm T}&gt;5.0$ GeV/$c$ and associate deuterons and anti-deuterons for 1.35-1.8 GeV/$c$.
description: CERN-LHC. Deuteron production in high-energy collisions is sensitive to the space-time evolution of the collision system, and is typically described by a coalescence mechanism. For the first time, we present results on jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV, providing an opportunity to test the established picture for deuteron production in events with a hard scattering. Using a trigger particle with high transverse-momentum~($p_{\rm T}&gt;5$ GeV/$c$) as a proxy for the presence of a jet at mid-rapidity, we observe a measurable population of deuterons being produced around the jet proxy. The associated deuteron yield measured in a narrow angular range around the trigger particle differs by 2--3 standard deviations from the uncorrelated background. The data are described by PYTHIA model calculations featuring baryon coalescence.
DOI: 10.17182/hepdata.105975.v1/t3
title: "Table 3" of "Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV"

description: The per-trigger associated yield versus $\Delta\varphi$ for charged particles with $p_{\rm T}&gt;5.0$ GeV/$c$ and associate deuterons and anti-deuterons for 1.8-2.4 GeV/$c$.
description: CERN-LHC. Deuteron production in high-energy collisions is sensitive to the space-time evolution of the collision system, and is typically described by a coalescence mechanism. For the first time, we present results on jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV, providing an opportunity to test the established picture for deuteron production in events with a hard scattering. Using a trigger particle with high transverse-momentum~($p_{\rm T}&gt;5$ GeV/$c$) as a proxy for the presence of a jet at mid-rapidity, we observe a measurable population of deuterons being produced around the jet proxy. The associated deuteron yield measured in a narrow angular range around the trigger particle differs by 2--3 standard deviations from the uncorrelated background. The data are described by PYTHIA model calculations featuring baryon coalescence.
DOI: 10.17182/hepdata.105975.v1/t4
title: "Table 4" of "Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV"

description: The per-trigger associated yield versus $\Delta\varphi$ for charged particles with $p_{\rm T}&gt;5.0$ GeV/$c$ and associate deuterons and anti-deuterons for 2.4-3.0 GeV/$c$.
description: CERN-LHC. Deuteron production in high-energy collisions is sensitive to the space-time evolution of the collision system, and is typically described by a coalescence mechanism. For the first time, we present results on jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV, providing an opportunity to test the established picture for deuteron production in events with a hard scattering. Using a trigger particle with high transverse-momentum~($p_{\rm T}&gt;5$ GeV/$c$) as a proxy for the presence of a jet at mid-rapidity, we observe a measurable population of deuterons being produced around the jet proxy. The associated deuteron yield measured in a narrow angular range around the trigger particle differs by 2--3 standard deviations from the uncorrelated background. The data are described by PYTHIA model calculations featuring baryon coalescence.
DOI: 10.17182/hepdata.105975.v1/t5
title: "Table 5" of "Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV"

description: The per-trigger associated yield versus $\Delta\varphi$ for charged particles with $p_{\rm T}&gt;5.0$ GeV/$c$ and associate deuterons and anti-deuterons for 3.0-4.0 GeV/$c$.
description: CERN-LHC. Deuteron production in high-energy collisions is sensitive to the space-time evolution of the collision system, and is typically described by a coalescence mechanism. For the first time, we present results on jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV, providing an opportunity to test the established picture for deuteron production in events with a hard scattering. Using a trigger particle with high transverse-momentum~($p_{\rm T}&gt;5$ GeV/$c$) as a proxy for the presence of a jet at mid-rapidity, we observe a measurable population of deuterons being produced around the jet proxy. The associated deuteron yield measured in a narrow angular range around the trigger particle differs by 2--3 standard deviations from the uncorrelated background. The data are described by PYTHIA model calculations featuring baryon coalescence.
DOI: 10.17182/hepdata.105975.v1/t6
title: "Table 6" of "Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV"

description: No table description available.
description: CERN-LHC. Deuteron production in high-energy collisions is sensitive to the space-time evolution of the collision system, and is typically described by a coalescence mechanism. For the first time, we present results on jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV, providing an opportunity to test the established picture for deuteron production in events with a hard scattering. Using a trigger particle with high transverse-momentum~($p_{\rm T}&gt;5$ GeV/$c$) as a proxy for the presence of a jet at mid-rapidity, we observe a measurable population of deuterons being produced around the jet proxy. The associated deuteron yield measured in a narrow angular range around the trigger particle differs by 2--3 standard deviations from the uncorrelated background. The data are described by PYTHIA model calculations featuring baryon coalescence.
DOI: 10.17182/hepdata.105998.v1/t1
title: "Table 5" of "Search for new phenomena in $pp$ collisions in final states with tau leptons, $b$-jets, and missing transverse momentum with the ATLAS detector"

description: Relative systematic uncertainties in the estimated number of background events in the signal regions. In the lower part of the table, a breakdown of the total uncertainty into different categories is given. For the multi-bin SR, the breakdown refers to the integral over all three $p_{\text{T}}(\tau)$ bins. As the individual uncertainties are correlated, they do not add in quadrature to equal the total background uncertainty.
description: A search for new phenomena in final states with hadronically decaying tau leptons, b-jets, and missing transverse momentum is presented. The analyzed dataset comprises pp collision data at a center-of-mass energy of 13 TeV with an integrated luminosity of 139/fb, delivered by the Large Hadron Collider and recorded with the ATLAS detector from 2015 to 2018. The observed data are compatible with the expected Standard Model background. The results are interpreted in simplified models for two different scenarios. The first model considers pair production of supersymmetric top squarks, each of which decays into a b-quark, a neutrino and a supersymmetric tau slepton. Each tau slepton in turn decays into a tau lepton and a nearly massless supersymmetric gravitino. Within this model, top-squark masses of 1.4 TeV can be excluded at the 95% confidence level over a wide range of tau-slepton masses. The second model considers pair production of leptoquarks with decays into third-generation leptons and quarks. Depending on the branching fraction into charged leptons, leptoquarks with masses up to around 1.25 TeV can be excluded at the 95% confidence level for the case of scalar leptoquarks and up to 1.8 TeV (1.5 TeV) for vector leptoquarks in a Yang–Mills (minimal-coupling) scenario. In addition, model-independent upper limits are set on the cross section of processes beyond the Standard Model.