cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.80046.v1/t66
title: "Table 66" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta\phi}$ measured in the helicity frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t67
title: "Table 67" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\phi}$ measured in the helicity frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t68
title: "Table 68" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The frame-invariant polarization parameter $\tilde{\lambda}$ measured in the helicity frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t69
title: "Table 69" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta}$ measured in the helicity frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t70
title: "Table 70" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta\phi}$ measured in the helicity frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t71
title: "Table 71" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\phi}$ measured in the helicity frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t72
title: "Table 72" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The frame-invariant polarization parameter $\tilde{\lambda}$ measured in the helicity frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t73
title: "Table 73" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta}$ measured in the Collins-Soper frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t74
title: "Table 74" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta\phi}$ measured in the Collins-Soper frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t75
title: "Table 75" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\phi}$ measured in the Collins-Soper frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t76
title: "Table 76" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The frame-invariant polarization parameter $\tilde{\lambda}$ measured in the Collins-Soper frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t77
title: "Table 77" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta}$ measured in the Collins-Soper frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t78
title: "Table 78" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta\phi}$ measured in the Collins-Soper frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t79
title: "Table 79" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\phi}$ measured in the Collins-Soper frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t80
title: "Table 80" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The frame-invariant polarization parameter $\tilde{\lambda}$ measured in the Collins-Soper frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t81
title: "Table 81" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta}$ measured in the Gottfried-Jackson frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t82
title: "Table 82" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta\phi}$ measured in the Gottfried-Jackson frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t83
title: "Table 83" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\phi}$ measured in the Gottfried-Jackson frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t84
title: "Table 84" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The frame-invariant polarization parameter $\tilde{\lambda}$ measured in the Gottfried-Jackson frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=7\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t85
title: "Table 85" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta}$ measured in the Gottfried-Jackson frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t86
title: "Table 86" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\theta\phi}$ measured in the Gottfried-Jackson frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t87
title: "Table 87" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The polarization parameter $\lambda_{\phi}$ measured in the Gottfried-Jackson frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t88
title: "Table 88" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: The frame-invariant polarization parameter $\tilde{\lambda}$ measured in the Gottfried-Jackson frame for the $\Upsilon(3S)$ state in different bins of $p_{T}^{\Upsilon}$ and three rapidity ranges using data collected at $\sqrt{s}=8\,\mathrm{TeV}$. The first uncertainty is statistical and the second represents the systematic uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t89
title: "Table 89" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: Values of the polarization parameter $\lambda_\theta$ measured in the helicity(SH), Collins-Soper(CS) and Gottfried-Jackson(TH) frames for the $\Upsilon(3S)$ produced at $\sqrt{s}=7$ TeV in the rapidity range $2.2 &lt; y^\Upsilon &lt; 4.5$ and different bins of $p_{T}^{\Upsilon}$. The first quoted uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t90
title: "Table 90" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: Values of the polarization parameter $\lambda_{\theta\phi}$ measured in the helicity(SH), Collins-Soper(CS) and Gottfried-Jackson(TH) frames for the $\Upsilon(3S)$ produced at $\sqrt{s}=7$ TeV in the rapidity range $2.2 &lt; y^\Upsilon &lt; 4.5$ and different bins of $p_{T}^{\Upsilon}$. The first quoted uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t92
title: "Table 92" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: Values of the frame-invariant polarization parameter $\tilde{\lambda}$ measured in the helicity(SH), Collins-Soper(CS) and Gottfried-Jackson(TH) frames for the $\Upsilon(3S)$ produced at $\sqrt{s}=7$ TeV in the rapidity range $2.2 &lt; y^\Upsilon &lt; 4.5$ and different bins of $p_{T}^{\Upsilon}$. The first quoted uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t91
title: "Table 91" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: Values of the polarization parameter $\lambda_{\phi}$ measured in the helicity(SH), Collins-Soper(CS) and Gottfried-Jackson(TH) frames for the $\Upsilon(3S)$ produced at $\sqrt{s}=7$ TeV in the rapidity range $2.2 &lt; y^\Upsilon &lt; 4.5$ and different bins of $p_{T}^{\Upsilon}$. The first quoted uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t93
title: "Table 93" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: Values of the polarization parameter $\lambda_{\theta}$ measured in the helicity(SH), Collins-Soper(CS) and Gottfried-Jackson(TH) frames for the $\Upsilon(3S)$ produced at $\sqrt{s}=8$ TeV in the rapidity range $2.2 &lt; y^\Upsilon &lt; 4.5$ and different bins of $p_{T}^{\Upsilon}$. The first quoted uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t94
title: "Table 94" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: Values of the polarization parameter $\lambda_{\theta\phi}$ measured in the helicity(SH), Collins-Soper(CS) and Gottfried-Jackson(TH) frames for the $\Upsilon(3S)$ produced at $\sqrt{s}=8$ TeV in the rapidity range $2.2 &lt; y^\Upsilon &lt; 4.5$ and different bins of $p_{T}^{\Upsilon}$. The first quoted uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t95
title: "Table 95" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: Values of the polarization parameter $\lambda_{\phi}$ measured in the helicity(SH), Collins-Soper(CS) and Gottfried-Jackson(TH) frames for the $\Upsilon(3S)$ produced at $\sqrt{s}=8$ TeV in the rapidity range $2.2 &lt; y^\Upsilon &lt; 4.5$ and different bins of $p_{T}^{\Upsilon}$. The first quoted uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80046.v1/t96
title: "Table 96" of "Measurement of the $\Upsilon$ polarization in $pp$ collisions at $\sqrt{s}$=7 and 8TeV"

description: Values of the frame-invariant polarization parameter $\tilde{\lambda}$ measured in the helicity(SH), Collins-Soper(CS) and Gottfried-Jackson(TH) frames for the $\Upsilon(3S)$ produced at $\sqrt{s}=8$ TeV in the rapidity range $2.2 &lt; y^\Upsilon &lt; 4.5$ and different bins of $p_{T}^{\Upsilon}$. The first quoted uncertainty is statistical and the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.80058.v1/t1
title: "Table 1" of "Measurement of the muon neutrino inclusive charged-current cross section in the energy range of 1-3 GeV with the T2K INGRID detector"

description: Results of the $\nu_{\mu}$ CC inclusive cross section on Fe.
description: No data abstract available.
DOI: 10.17182/hepdata.80076.v1/t1
title: "Table 1" of "Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Cross section for the production of W bosons for different inclusive jet multiplicities.
description: CERN-LHC.
This paper presents a measurement of the W boson production cross section and the W+/W- cross-section ratio, both in association with jets, in proton-proton collisions at sqrt(s) = 8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb^-1. Differential cross sections for events with at least one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W+/W- the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proton.
DOI: 10.17182/hepdata.80076.v1/t2
title: "Table 2" of "Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Statistical correlation between bins in data for the cross section for the production of W bosons for different inclusive jet multiplicities.
description: CERN-LHC.
This paper presents a measurement of the W boson production cross section and the W+/W- cross-section ratio, both in association with jets, in proton-proton collisions at sqrt(s) = 8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb^-1. Differential cross sections for events with at least one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W+/W- the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proton.
DOI: 10.17182/hepdata.80076.v1/t3
title: "Table 3" of "Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the inclusive jet multiplicity.
description: CERN-LHC.
This paper presents a measurement of the W boson production cross section and the W+/W- cross-section ratio, both in association with jets, in proton-proton collisions at sqrt(s) = 8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb^-1. Differential cross sections for events with at least one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W+/W- the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proton.
DOI: 10.17182/hepdata.80076.v1/t4
title: "Table 4" of "Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the inclusive jet multiplicity.
description: CERN-LHC.
This paper presents a measurement of the W boson production cross section and the W+/W- cross-section ratio, both in association with jets, in proton-proton collisions at sqrt(s) = 8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb^-1. Differential cross sections for events with at least one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W+/W- the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proton.
DOI: 10.17182/hepdata.80076.v1/t5
title: "Table 5" of "Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the inclusive jet multiplicity.
description: CERN-LHC.
This paper presents a measurement of the W boson production cross section and the W+/W- cross-section ratio, both in association with jets, in proton-proton collisions at sqrt(s) = 8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb^-1. Differential cross sections for events with at least one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W+/W- the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proton.