cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.129068.v1/t10
title: "Table 4.4" of "Production of $\Lambda$ and ${\rm K}^{0}_{\rm S}$ in jets in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5$ TeV and pp collisions at $\sqrt{s} = 7$ TeV"

description: The $p_{\rm T}$ dependent $(\Lambda+\overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ of ${\rm V}^{0}$ particles produced in jets with $p_{\rm T,jet}&gt;10$ GeV/$c$ p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and in pp collisions at $\sqrt{s} = 7$ TeV.
description: 'The production of $\Lambda$ baryons and ${\rm K}_{\rm S}^{0}$ mesons (${\rm V}^{0}$ particles) was measured in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and pp collisions at $\sqrt{s} = 7$ TeV with ALICE at the LHC. The production of these strange particles is studied separately for particles associated with hard scatterings and the underlying event to shed light on the baryon-to-meson ratio enhancement observed at intermediate transverse momentum ($p_{\rm T}$) in high multiplicity pp and p-Pb collisions. Hard scatterings are selected on an event-by-event basis with jets reconstructed with the anti-$k_{\rm T}$ algorithm using charged particles. The production of strange particles associated with jets $p_{\rm T,jet}^{\rm ch} &gt; 10$ GeV/$c$ is reported as a function of $p_{\rm T}$ in both systems; and its dependence on $p_{\rm T}$ with jets $p_{\rm T,jet}^{\rm ch} &gt; 20$ GeV/$c$ and on angular distance from the jet axis, $R({\rm V}^{0},{\rm jet})$, for jets with $p_{\rm T,jet}^{\rm ch} &gt; 10$ GeV/$c$ are reported in p-Pb collisions. The results are compared with the strange particle production in the underlying event. The $\Lambda/{\rm K}_{\rm S}^{0}$ ratio associated with jets in p-Pb collisions for $R({\rm V}^{0},{\rm jet}) &lt; 0.4$ is consistent with the ratio measured in pp collisions and with the expectation of jets fragmenting in vacuum given by the PYTHIA event generator.'
DOI: 10.17182/hepdata.129068.v1/t11
title: "Table 4.5" of "Production of $\Lambda$ and ${\rm K}^{0}_{\rm S}$ in jets in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5$ TeV and pp collisions at $\sqrt{s} = 7$ TeV"

description: The $p_{\rm T}$ dependent $(\Lambda+\overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ of ${\rm V}^{0}$ particles produced in jets with $p_{\rm T,jet}&gt;20$ GeV/$c$ p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: 'The production of $\Lambda$ baryons and ${\rm K}_{\rm S}^{0}$ mesons (${\rm V}^{0}$ particles) was measured in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and pp collisions at $\sqrt{s} = 7$ TeV with ALICE at the LHC. The production of these strange particles is studied separately for particles associated with hard scatterings and the underlying event to shed light on the baryon-to-meson ratio enhancement observed at intermediate transverse momentum ($p_{\rm T}$) in high multiplicity pp and p-Pb collisions. Hard scatterings are selected on an event-by-event basis with jets reconstructed with the anti-$k_{\rm T}$ algorithm using charged particles. The production of strange particles associated with jets $p_{\rm T,jet}^{\rm ch} &gt; 10$ GeV/$c$ is reported as a function of $p_{\rm T}$ in both systems; and its dependence on $p_{\rm T}$ with jets $p_{\rm T,jet}^{\rm ch} &gt; 20$ GeV/$c$ and on angular distance from the jet axis, $R({\rm V}^{0},{\rm jet})$, for jets with $p_{\rm T,jet}^{\rm ch} &gt; 10$ GeV/$c$ are reported in p-Pb collisions. The results are compared with the strange particle production in the underlying event. The $\Lambda/{\rm K}_{\rm S}^{0}$ ratio associated with jets in p-Pb collisions for $R({\rm V}^{0},{\rm jet}) &lt; 0.4$ is consistent with the ratio measured in pp collisions and with the expectation of jets fragmenting in vacuum given by the PYTHIA event generator.'
DOI: 10.17182/hepdata.129068.v1/t8
title: "Table 4.2" of "Production of $\Lambda$ and ${\rm K}^{0}_{\rm S}$ in jets in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5$ TeV and pp collisions at $\sqrt{s} = 7$ TeV"

description: The $p_{\rm T}$ dependent $(\Lambda+\overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ of ${\rm V}^{0}$ particles in underlying events in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
description: 'The production of $\Lambda$ baryons and ${\rm K}_{\rm S}^{0}$ mesons (${\rm V}^{0}$ particles) was measured in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and pp collisions at $\sqrt{s} = 7$ TeV with ALICE at the LHC. The production of these strange particles is studied separately for particles associated with hard scatterings and the underlying event to shed light on the baryon-to-meson ratio enhancement observed at intermediate transverse momentum ($p_{\rm T}$) in high multiplicity pp and p-Pb collisions. Hard scatterings are selected on an event-by-event basis with jets reconstructed with the anti-$k_{\rm T}$ algorithm using charged particles. The production of strange particles associated with jets $p_{\rm T,jet}^{\rm ch} &gt; 10$ GeV/$c$ is reported as a function of $p_{\rm T}$ in both systems; and its dependence on $p_{\rm T}$ with jets $p_{\rm T,jet}^{\rm ch} &gt; 20$ GeV/$c$ and on angular distance from the jet axis, $R({\rm V}^{0},{\rm jet})$, for jets with $p_{\rm T,jet}^{\rm ch} &gt; 10$ GeV/$c$ are reported in p-Pb collisions. The results are compared with the strange particle production in the underlying event. The $\Lambda/{\rm K}_{\rm S}^{0}$ ratio associated with jets in p-Pb collisions for $R({\rm V}^{0},{\rm jet}) &lt; 0.4$ is consistent with the ratio measured in pp collisions and with the expectation of jets fragmenting in vacuum given by the PYTHIA event generator.'
DOI: 10.17182/hepdata.129068.v1/t9
title: "Table 4.3" of "Production of $\Lambda$ and ${\rm K}^{0}_{\rm S}$ in jets in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5$ TeV and pp collisions at $\sqrt{s} = 7$ TeV"

description: The $p_{\rm T}$ dependent $(\Lambda+\overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ of ${\rm V}^{0}$ particles in underlying events and that selected with $R({\rm V}^{0},{\rm jet})&lt;0.4$ in pp collisions at $\sqrt{s} = 7$ TeV.
description: 'The production of $\Lambda$ baryons and ${\rm K}_{\rm S}^{0}$ mesons (${\rm V}^{0}$ particles) was measured in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and pp collisions at $\sqrt{s} = 7$ TeV with ALICE at the LHC. The production of these strange particles is studied separately for particles associated with hard scatterings and the underlying event to shed light on the baryon-to-meson ratio enhancement observed at intermediate transverse momentum ($p_{\rm T}$) in high multiplicity pp and p-Pb collisions. Hard scatterings are selected on an event-by-event basis with jets reconstructed with the anti-$k_{\rm T}$ algorithm using charged particles. The production of strange particles associated with jets $p_{\rm T,jet}^{\rm ch} &gt; 10$ GeV/$c$ is reported as a function of $p_{\rm T}$ in both systems; and its dependence on $p_{\rm T}$ with jets $p_{\rm T,jet}^{\rm ch} &gt; 20$ GeV/$c$ and on angular distance from the jet axis, $R({\rm V}^{0},{\rm jet})$, for jets with $p_{\rm T,jet}^{\rm ch} &gt; 10$ GeV/$c$ are reported in p-Pb collisions. The results are compared with the strange particle production in the underlying event. The $\Lambda/{\rm K}_{\rm S}^{0}$ ratio associated with jets in p-Pb collisions for $R({\rm V}^{0},{\rm jet}) &lt; 0.4$ is consistent with the ratio measured in pp collisions and with the expectation of jets fragmenting in vacuum given by the PYTHIA event generator.'
DOI: 10.17182/hepdata.129088.v1/t1
title: "Figure 1" of "Measurement of Direct-Photon Cross Section and Double-Helicity Asymmetry at $\sqrt{s}=510$ GeV in $\vec{p}+\vec{p}$ Collisions"

description: Cross sections for inclusive and isolated direct photons as a function of $p_T$. Not shown are 10% absolute luminosity uncertainties.
description: BNL-RHIC. We present the measurement of the cross section and double helicity asymmetry $A_{LL}$ of direct photon production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}$ = 510 GeV. The measurement has been performed at midrapidity ($|\eta| &lt;$ 0.25) with the PHENIX detector at the Relativistic Heavy Ion Collider. Direct photons are dominantly produced by the quark-gluon scattering at relativistic energies. Since direct photons are produced from the initial partonic hard scattering and do not interact via the strong force, this measurement provides a clean and direct access to the gluons in the polarized proton in the gluon momentum fraction range 0.02 $&lt; x &lt;$ 0.08.
DOI: 10.17182/hepdata.129088.v1/t2
title: "Figure 2" of "Measurement of Direct-Photon Cross Section and Double-Helicity Asymmetry at $\sqrt{s}=510$ GeV in $\vec{p}+\vec{p}$ Collisions"

description: Double helicity asymmetry $A_{LL}$ $vs$ $p_{T}$ for isolated direct-photon production in polarized $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=510$ GeV at midrapidity. Not shown are $3.9 \times 10^{-4}$ shift uncertainty from relative luminosity and 6.6% scale uncertainty from polarization.
description: BNL-RHIC. We present the measurement of the cross section and double helicity asymmetry $A_{LL}$ of direct photon production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}$ = 510 GeV. The measurement has been performed at midrapidity ($|\eta| &lt;$ 0.25) with the PHENIX detector at the Relativistic Heavy Ion Collider. Direct photons are dominantly produced by the quark-gluon scattering at relativistic energies. Since direct photons are produced from the initial partonic hard scattering and do not interact via the strong force, this measurement provides a clean and direct access to the gluons in the polarized proton in the gluon momentum fraction range 0.02 $&lt; x &lt;$ 0.08.
DOI: 10.25549/vercoutere-ouc110611331
title: 2 people holding hands in front of a military man

description: One red nude male with white highlights depicted from neck to knees is holding hands with the blue arm of a person who is otherwise not in view. They are standing in front of a man dressed in a blue military uniform and brown shoes depicted from neck to shoes. Background is turquoise bricks outlined in red. See description of 001 for OT notes.
DOI: 10.25549/vercoutere-ouc110611350
title: Nude woman seated next to a man in a suit

description: One olive green and tan female depicted from head to waist is seated next to a male in a brown suit outline in black who is depicted from neck to knees. A large brown and orange dish is between the two figures. Gray bars are to the female's right. The background is red, brown, gray, and black. See description of 001 for OT notes.
DOI: 10.25549/vercoutere-ouc113056794
title: Publisher correspondence

description: Correspondence between Al Vercoutere and various publishers related to publication of patient artwork in textbooks. Arranged in chronological order includes letters and forms (101), check receipts (9), and envelopes (15)
DOI: 10.25549/vercoutere-ouc113056802
title: Publisher correspondence

description: Correspondence between Al Vercoutere and various publishers related to publication of patient artwork in textbooks. Arranged in chronological order includes letters and forms (101), check receipts (9), and envelopes (15)
DOI: 10.25549/vercoutere-ouc113056800
title: Publisher correspondence

description: Correspondence between Al Vercoutere and various publishers related to publication of patient artwork in textbooks. Arranged in chronological order includes letters and forms (101), check receipts (9), and envelopes (15)
DOI: 10.17182/hepdata.129151.v1/t1
title: "Table 1" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: Comparisons of the data and the expected background distributions of the WZ invariant mass in the Drell-Yan signal region. The background predictions are obtained through a background-only simultaneous fit to the Drell-Yan signal region and the WZ-QCD Drell-Yan and ZZ Drell-Yan control regions. The yields are normalized to the bin width.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t2
title: "Table 2" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: Comparisons of the data and the expected background distributions of the WZ invariant mass in the ANN-based VBF signal region. The background predictions are obtained through a background-only simultaneous fit to the VBF signal region and the WZ-QCD and ZZ VBF control regions. The yields are normalized to the bin width
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t3
title: "Table 3" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: Comparisons of the observed data and the expected background distributions of the WZ invariant mass using the cut-based VBF selection. The background predictions are obtained through a background-only simultaneous fit to the VBF cut-based signal region and the WZ-QCD and ZZ VBF control regions. The yields are normalized to the bin width.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t4
title: "Table 4" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: Drell-Yan signal region selection cutflow for a simulated W' in the HVT model A with m_W' = 1 TeV. The unweighted number of events is shown.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t10
title: "Table 10" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: The acceptancetimes efficiencyof VBF H5+ selection after the cut-based VBF selection at different mass points for the individual channels and the sum of all channels. The uncertainty includes both statistical and experimental systematic components.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t11
title: "Table 11" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: The acceptancetimes efficiencyof VBF HVT W' selection after the cut-based VBF selection at different mass points for the individual channels and the sum of all channels. The uncertainty includes both statistical and experimental systematic components.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t5
title: "Table 5" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: VBF signal region selection cutflow for a simulated W' in the HVT model C with m_W' = 500 GeV. The unweighted number of events is shown.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t6
title: "Table 6" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: VBF signal region selection cutflow for a simulated H5+ in the GM model with m_H5+ = 450 GeV. The unweighted number of events is shown.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t12
title: "Table 12" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: Observed and expected 95% CL exclusion upper limits on sigma * B(W' -&gt; WZ) for the Drell-Yan production of a W' boson in the HVT model as a function of its mass. The LO theory predictions for HVT Model A with g_V=1 and Model B with g_V=$ are also shown.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t14
title: "Table 14" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: Using the ANN VBF selection, observed and expected 95% CL upper limits on sigma * B(W' -&gt; WZ) of the GM model as a function of m_H_5.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.
DOI: 10.17182/hepdata.129151.v1/t8
title: "Table 8" of "Search for resonant $WZ \rightarrow \ell\nu \ell^{\prime}\ell^{\prime}$ production in proton$-$proton collisions at $\mathbf{\sqrt{s} = 13}$ TeV with the ATLAS detector"

description: The acceptancetimes efficiencyof VBF H5+ selection after the ANN-based VBF selection at different mass points for the individual channels and the sum of all channels. The uncertainty includes both statistical and experimental systematic components.
description: A search for a WZ resonance, in the fully leptonic final state (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process. No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.