cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79407.v1/t10
title: "Table 10" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 5, left, subfigur a, Upper limits at 95% CL on the Higgs boson production cross section times branching fraction in the evmuv channel, for ggF signals with narrow-width lineshape as a function of the signal mass.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t11
title: "Table 11" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 5, right, subfigure b, Upper limits at 95% CL on the Higgs boson production cross section times branching fraction in the evmuv channel, for VBF signals with narrow-width lineshape as a function of the signal mass.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t12
title: "Table 12" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 6, Upper limits at 95% CL on the total ggF and VBF Higgs boson production cross section times branching fraction in the evmuv channel, for a signal at 800 GeV as a function of the ggF cross section divided by the combined ggF and VBF production cross section.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t13
title: "Table 13" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 9, top left, subfigure a, Upper limits at 95% CL on the Higgs boson production cross section times branching fraction for a signal with a width of 15% of the mass for the ggF production.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t14
title: "Table 14" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 9, top right, subfigure b, Upper limits at 95% CL on the Higgs boson production cross section times branching fraction for a signal with a width of 15% of the mass for the VBF production.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t15
title: "Table 15" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 10, left, subfigure a, Upper limits at 95% CL on the resonance production cross section times branching fraction for a GM signal.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t9
title: "Table 9" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 4, bottom, subfigure c, post-fit distributions of the transverse mass mT in the VBF2Jet Signal region. The "0" value means lack of statistics.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t16
title: "Table 16" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 11, left, subfigure a, Upper limits at 95% CL on the resonance production cross section times branching fraction for a HVT qqA signal.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t17
title: "Table 17" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 11, right, subfigure b, Upper limits at 95% CL on the resonance production cross section times branching fraction for a HVT VBF signal.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t18
title: "Table 18" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 12, bottom, subfigure c, Upper limits at 95% CL on the resonance production cross section times branching fraction for an EML spin-2 VBF signal.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t19
title: "Table 19" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 12, top right, subfigure b, Upper limits at 95% CL on the resonance production cross section times branching fraction for a graviton signal with coupling parameter equals 0.5
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t20
title: "Table 20" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Figure 12, top left, subfigure a, Upper limits at 95% CL on the resonance production cross section times branching fraction for a graviton signal with coupling parameter equals 1.0
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t21
title: "Table 21" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 2e, Event selection efficiencies in the VBF2J event categories as a function of the signal mass for the ggF or qqA production. The "0" efficiency mass point means there's no such signal sample for the corresponding model.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t23
title: "Table 23" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 2c, Event selection efficiencies in the VBF1J event categories as a function of the signal mass for the ggF or qqA production. The "0" efficiency mass point means there's no such signal sample for the corresponding model.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t22
title: "Table 22" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 2f, Event selection efficiencies in the VBF2J event categories for different kinds of VBF signals production. The "0" efficiency mass point means there's no such signal sample for the corresponding model.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t24
title: "Table 24" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 2d, Event selection efficiencies in the VBF1J event categories for different kinds of VBF signals production. The "0" efficiency mass point means there's no such signal sample for the corresponding model.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t25
title: "Table 25" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 2a, Event selection efficiencies in the ggF event categories as a function of the signal mass for the ggF or qqA production. The "0" efficiency mass point means there's no such signal sample for the corresponding model.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t26
title: "Table 26" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 2b, Event selection efficiencies in the ggF event categories for different kinds of VBF signals production. The "0" efficiency mass point means there's no such signal sample for the corresponding model.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t27
title: "Table 27" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 6a, Upper limits at 95% CL on the Higgs production cross section times branching fraction in the evmuv channel, for a signal with a width of 5% of the mass for the ggF production.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t28
title: "Table 28" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 6c, Upper limits at 95% CL on the Higgs production cross section times branching fraction in the evmuv channel, for a signal with a width of 10% of the mass for the ggF production.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t29
title: "Table 29" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 6b, Upper limits at 95% CL on the Higgs production cross section times branching fraction in the evmuv channel, for a signal with a width of 5% of the mass for the VBF production.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t30
title: "Table 30" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 6d, Upper limits at 95% CL on the Higgs production cross section times branching fraction in the evmuv channel, for a signal with a width of 10% of the mass for the VBF production.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t31
title: "Table 31" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 7b, Upper limits at 95% CL on the total ggF and VBF Higgs production cross section times branching fraction for a signal at 1.8 TeV as a function of the ggF cross section over the combined ggF and VBF production cross section.
description: No data abstract available.
DOI: 10.17182/hepdata.79407.v1/t32
title: "Table 32" of "Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Auxiliary material Figure 7a, Upper limits at 95% CL on the total ggF and VBF Higgs production cross section times branching fraction for a signal at 200 GeV as a function of the ggF cross section over the combined ggF and VBF production cross section.
description: No data abstract available.
DOI: 10.17182/hepdata.79410.v1/t1
title: "Table 1" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t2
title: "Table 7" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Statistical correlation matrix from unfolding
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t3
title: "Table 2" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t4
title: "Table 8" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Statistical correlation matrix from unfolding
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t5
title: "Table 3" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t6
title: "Table 9" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Statistical correlation matrix from unfolding
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t7
title: "Table 4" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t10
title: "Table 11" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Statistical correlation matrix from unfolding
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t12
title: "Table 12" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Statistical correlation matrix from unfolding
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t14
title: "Table 14" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Electroweak correction factor to triple-differential dijet cross section
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.
DOI: 10.17182/hepdata.79410.v1/t8
title: "Table 10" of "Measurement of the triple-differential dijet cross section in proton-proton collisions at sqrt(s) = 8 TeV and constraints on parton distribution functions"

description: Statistical correlation matrix from unfolding
description: A measurement is presented of the triple-differential dijet cross section at a centre-of-mass energy of 8 TeV using 19.7 fb$^-1$ of data collected with the CMS detector in proton-proton collisions at the LHC. The cross section is measured as a function of the average transverse momentum, half the rapidity separation, and the boost of the two leading jets in the event. The cross section is corrected for detector effects and compared to calculations in perturbative quantum chromodynamics at next-to-leading order accuracy, complemented with electroweak and nonperturbative corrections. New constraints on parton distribution functions are obtained and the inferred value of the strong coupling constant is $\alpha_s(M_{Z})$ = 0.1199 $\pm$ 0.0015 (exp)$^{+0.0031}_{-0.0020}$ (theo), where M$_{Z}$ is the mass of the Z boson.