cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83194.v1/t3
title: "Table 3" of "Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV"

description: Upper limits at the 95% CL for a spin-2 resonance decaying to HH
description: Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV. The 95% CL upper limits on the production cross section times branching fraction on the resonant (spin-0 and spin-2) and nonresonant (anomalous trilinear Higgs boson coupling lambda_HHH and top Yukawa coupling yt, and EFT shape benchmarks) are provided.
DOI: 10.17182/hepdata.83194.v1/t4
title: "Table 4" of "Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV"

description: Upper limits at the 95% CL for nonresonant HH production with anomalous couplings (shape benchmarks)
description: Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV. The 95% CL upper limits on the production cross section times branching fraction on the resonant (spin-0 and spin-2) and nonresonant (anomalous trilinear Higgs boson coupling lambda_HHH and top Yukawa coupling yt, and EFT shape benchmarks) are provided.
DOI: 10.17182/hepdata.83194.v1/t5
title: "Table 5" of "Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV"

description: Upper limits at the 95% CL for for a spin-0 resonance decaying to HH, compared for the decay channels investigated
description: Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV. The 95% CL upper limits on the production cross section times branching fraction on the resonant (spin-0 and spin-2) and nonresonant (anomalous trilinear Higgs boson coupling lambda_HHH and top Yukawa coupling yt, and EFT shape benchmarks) are provided.
DOI: 10.17182/hepdata.83194.v1/t6
title: "Table 6" of "Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV"

description: Upper limits at the 95% CL for for a spin-0 resonance decaying to HH, compared for the event categories investigated
description: Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV. The 95% CL upper limits on the production cross section times branching fraction on the resonant (spin-0 and spin-2) and nonresonant (anomalous trilinear Higgs boson coupling lambda_HHH and top Yukawa coupling yt, and EFT shape benchmarks) are provided.
DOI: 10.17182/hepdata.83194.v1/t7
title: "Table 7" of "Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV"

description: Upper limits at the 95% CL for nonresonant HH production with anomalous lambda_HHH and yt couplings, compared for the decay channels investigated
description: Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV. The 95% CL upper limits on the production cross section times branching fraction on the resonant (spin-0 and spin-2) and nonresonant (anomalous trilinear Higgs boson coupling lambda_HHH and top Yukawa coupling yt, and EFT shape benchmarks) are provided.
DOI: 10.17182/hepdata.83194.v1/t8
title: "Table 8" of "Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV"

description: Upper limits at the 95% CL for nonresonant HH production with anomalous lambda_HHH and yt couplings, compared for the event categories investigated
description: Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at sqrt(s) = 13 TeV. The 95% CL upper limits on the production cross section times branching fraction on the resonant (spin-0 and spin-2) and nonresonant (anomalous trilinear Higgs boson coupling lambda_HHH and top Yukawa coupling yt, and EFT shape benchmarks) are provided.
DOI: 10.17182/hepdata.83195.v1/t1
title: "Figure 2a" of "Search for resonant and nonresonant Higgs boson pair production in the bblnulnu final state in proton-proton collisions at sqrt(s) = 13 TeV"

description: The dijet pT distributions in data and simulated events after requiring two leptons, two b-tagged jets, and 12 &lt; m_ll &lt; mZ − 15 GeV, for e+e- events. The various signal hypotheses displayed have been scaled to a cross section of 5 pb for display purposes.
description: CERN-LHC. Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into lnulnu, through either W or Z bosons, and bbbar. Based on a sample of proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb−1.

The main background processes, in decreasing order of importance, are ttbar, Drell-Yan, and single top quark production. 
Diboson, triboson, ttV and SM single Higgs boson production are also considered. 
Other contributions, such as W+jets or QCD multijet events with jets misidentified as leptons, are negligible.
Background simulation samples have been generated at NLO in QCD using powheg and MadGraph5 amc@nlo with FxFx merging and MadSpin. 
The signal samples of gluon fusion production of two Higgs bosons, and of spin-0 or spin-2 narrow resonances decaying into two Higgs bosons, have been generated at leading order (LO) in QCD using MadGraph5 amc@nlo version 2.2.2.0. 
The event generators used for both signal and background samples are interfaced with pythia 8.212.
The NNPDF 3.0 LO and NLO Parton Distribution Functions (PDF) are used.
Jets are reconstructed using a particle flow (PF) technique.
PF candidates are clustered to form jets using the anti-kT clustering algorithm with a distance parameter of 0.4.

Region of interest is defined as:
 - two leptons and two b-tagged jets
 - (Pt_l1, Pt_l2) &gt; (25GeV,15GeV) for the ee and mue channels 
 - (Pt_l1, Pt_l2) &gt; (20GeV,10GeV) for the mumu channel
 - (Pt_l1, Pt_l2) &gt; (25GeV,10GeV) for the emu channel
 - abs(eta_mu) &lt; 2.4
 - abs(eta_el) &lt; 2.5
 - pT_jet &gt; 20GeV
 - abs(eta_jet) &lt; 2.4
 - Delta_R(jet,lepton)&gt;0.3
 - 12 &lt; m_ll &lt; mZ −15 GeV
DOI: 10.17182/hepdata.83195.v1/t2
title: "Figure 2b" of "Search for resonant and nonresonant Higgs boson pair production in the bblnulnu final state in proton-proton collisions at sqrt(s) = 13 TeV"

description: The dijet pT distributions in data and simulated events after requiring two leptons, two b-tagged jets, and 12 &lt; m_ll &lt; mZ − 15 GeV, for e+mu- and e-mu+ events. The various signal hypotheses displayed have been scaled to a cross section of 5 pb for display purposes.
description: CERN-LHC. Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into lnulnu, through either W or Z bosons, and bbbar. Based on a sample of proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb−1.

The main background processes, in decreasing order of importance, are ttbar, Drell-Yan, and single top quark production. 
Diboson, triboson, ttV and SM single Higgs boson production are also considered. 
Other contributions, such as W+jets or QCD multijet events with jets misidentified as leptons, are negligible.
Background simulation samples have been generated at NLO in QCD using powheg and MadGraph5 amc@nlo with FxFx merging and MadSpin. 
The signal samples of gluon fusion production of two Higgs bosons, and of spin-0 or spin-2 narrow resonances decaying into two Higgs bosons, have been generated at leading order (LO) in QCD using MadGraph5 amc@nlo version 2.2.2.0. 
The event generators used for both signal and background samples are interfaced with pythia 8.212.
The NNPDF 3.0 LO and NLO Parton Distribution Functions (PDF) are used.
Jets are reconstructed using a particle flow (PF) technique.
PF candidates are clustered to form jets using the anti-kT clustering algorithm with a distance parameter of 0.4.

Region of interest is defined as:
 - two leptons and two b-tagged jets
 - (Pt_l1, Pt_l2) &gt; (25GeV,15GeV) for the ee and mue channels 
 - (Pt_l1, Pt_l2) &gt; (20GeV,10GeV) for the mumu channel
 - (Pt_l1, Pt_l2) &gt; (25GeV,10GeV) for the emu channel
 - abs(eta_mu) &lt; 2.4
 - abs(eta_el) &lt; 2.5
 - pT_jet &gt; 20GeV
 - abs(eta_jet) &lt; 2.4
 - Delta_R(jet,lepton)&gt;0.3
 - 12 &lt; m_ll &lt; mZ −15 GeV
DOI: 10.17182/hepdata.83195.v1/t3
title: "Figure 2c" of "Search for resonant and nonresonant Higgs boson pair production in the bblnulnu final state in proton-proton collisions at sqrt(s) = 13 TeV"

description: The dijet pT distributions in data and simulated events after requiring two leptons, two b-tagged jets, and 12 &lt; m_ll &lt; mZ − 15 GeV, for mu+mu- events. The various signal hypotheses displayed have been scaled to a cross section of 5 pb for display purposes.
description: CERN-LHC. Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into lnulnu, through either W or Z bosons, and bbbar. Based on a sample of proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb−1.

The main background processes, in decreasing order of importance, are ttbar, Drell-Yan, and single top quark production. 
Diboson, triboson, ttV and SM single Higgs boson production are also considered. 
Other contributions, such as W+jets or QCD multijet events with jets misidentified as leptons, are negligible.
Background simulation samples have been generated at NLO in QCD using powheg and MadGraph5 amc@nlo with FxFx merging and MadSpin. 
The signal samples of gluon fusion production of two Higgs bosons, and of spin-0 or spin-2 narrow resonances decaying into two Higgs bosons, have been generated at leading order (LO) in QCD using MadGraph5 amc@nlo version 2.2.2.0. 
The event generators used for both signal and background samples are interfaced with pythia 8.212.
The NNPDF 3.0 LO and NLO Parton Distribution Functions (PDF) are used.
Jets are reconstructed using a particle flow (PF) technique.
PF candidates are clustered to form jets using the anti-kT clustering algorithm with a distance parameter of 0.4.

Region of interest is defined as:
 - two leptons and two b-tagged jets
 - (Pt_l1, Pt_l2) &gt; (25GeV,15GeV) for the ee and mue channels 
 - (Pt_l1, Pt_l2) &gt; (20GeV,10GeV) for the mumu channel
 - (Pt_l1, Pt_l2) &gt; (25GeV,10GeV) for the emu channel
 - abs(eta_mu) &lt; 2.4
 - abs(eta_el) &lt; 2.5
 - pT_jet &gt; 20GeV
 - abs(eta_jet) &lt; 2.4
 - Delta_R(jet,lepton)&gt;0.3
 - 12 &lt; m_ll &lt; mZ −15 GeV
DOI: 10.17182/hepdata.83195.v1/t4
title: "Figure 4a" of "Search for resonant and nonresonant Higgs boson pair production in the bblnulnu final state in proton-proton collisions at sqrt(s) = 13 TeV"

description: The mjj distribution in data and simulated events after requiring all selection criteria in the e+e- channel. The various signal hypotheses displayed have been scaled to a cross section of 5 pb for display purposes.
description: CERN-LHC. Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into lnulnu, through either W or Z bosons, and bbbar. Based on a sample of proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb−1.

The main background processes, in decreasing order of importance, are ttbar, Drell-Yan, and single top quark production. 
Diboson, triboson, ttV and SM single Higgs boson production are also considered. 
Other contributions, such as W+jets or QCD multijet events with jets misidentified as leptons, are negligible.
Background simulation samples have been generated at NLO in QCD using powheg and MadGraph5 amc@nlo with FxFx merging and MadSpin. 
The signal samples of gluon fusion production of two Higgs bosons, and of spin-0 or spin-2 narrow resonances decaying into two Higgs bosons, have been generated at leading order (LO) in QCD using MadGraph5 amc@nlo version 2.2.2.0. 
The event generators used for both signal and background samples are interfaced with pythia 8.212.
The NNPDF 3.0 LO and NLO Parton Distribution Functions (PDF) are used.
Jets are reconstructed using a particle flow (PF) technique.
PF candidates are clustered to form jets using the anti-kT clustering algorithm with a distance parameter of 0.4.

Region of interest is defined as:
 - two leptons and two b-tagged jets
 - (Pt_l1, Pt_l2) &gt; (25GeV,15GeV) for the ee and mue channels 
 - (Pt_l1, Pt_l2) &gt; (20GeV,10GeV) for the mumu channel
 - (Pt_l1, Pt_l2) &gt; (25GeV,10GeV) for the emu channel
 - abs(eta_mu) &lt; 2.4
 - abs(eta_el) &lt; 2.5
 - pT_jet &gt; 20GeV
 - abs(eta_jet) &lt; 2.4
 - Delta_R(jet,lepton)&gt;0.3
 - 12 &lt; m_ll &lt; mZ −15 GeV
DOI: 10.17182/hepdata.83195.v1/t5
title: "Figure 4b" of "Search for resonant and nonresonant Higgs boson pair production in the bblnulnu final state in proton-proton collisions at sqrt(s) = 13 TeV"

description: The mjj distribution in data and simulated events after requiring all selection criteria in the e^{+/-}mu^{-/+} channel. The various signal hypotheses displayed have been scaled to a cross section of 5 pb for display purposes.
description: CERN-LHC. Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into lnulnu, through either W or Z bosons, and bbbar. Based on a sample of proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb−1.

The main background processes, in decreasing order of importance, are ttbar, Drell-Yan, and single top quark production. 
Diboson, triboson, ttV and SM single Higgs boson production are also considered. 
Other contributions, such as W+jets or QCD multijet events with jets misidentified as leptons, are negligible.
Background simulation samples have been generated at NLO in QCD using powheg and MadGraph5 amc@nlo with FxFx merging and MadSpin. 
The signal samples of gluon fusion production of two Higgs bosons, and of spin-0 or spin-2 narrow resonances decaying into two Higgs bosons, have been generated at leading order (LO) in QCD using MadGraph5 amc@nlo version 2.2.2.0. 
The event generators used for both signal and background samples are interfaced with pythia 8.212.
The NNPDF 3.0 LO and NLO Parton Distribution Functions (PDF) are used.
Jets are reconstructed using a particle flow (PF) technique.
PF candidates are clustered to form jets using the anti-kT clustering algorithm with a distance parameter of 0.4.

Region of interest is defined as:
 - two leptons and two b-tagged jets
 - (Pt_l1, Pt_l2) &gt; (25GeV,15GeV) for the ee and mue channels 
 - (Pt_l1, Pt_l2) &gt; (20GeV,10GeV) for the mumu channel
 - (Pt_l1, Pt_l2) &gt; (25GeV,10GeV) for the emu channel
 - abs(eta_mu) &lt; 2.4
 - abs(eta_el) &lt; 2.5
 - pT_jet &gt; 20GeV
 - abs(eta_jet) &lt; 2.4
 - Delta_R(jet,lepton)&gt;0.3
 - 12 &lt; m_ll &lt; mZ −15 GeV
DOI: 10.17182/hepdata.83195.v1/t6
title: "Figure 4c" of "Search for resonant and nonresonant Higgs boson pair production in the bblnulnu final state in proton-proton collisions at sqrt(s) = 13 TeV"

description: The mjj distribution in data and simulated events after requiring all selection criteria in the mu+mu- channel. The various signal hypotheses displayed have been scaled to a cross section of 5 pb for display purposes.
description: CERN-LHC. Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into lnulnu, through either W or Z bosons, and bbbar. Based on a sample of proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb−1.

The main background processes, in decreasing order of importance, are ttbar, Drell-Yan, and single top quark production. 
Diboson, triboson, ttV and SM single Higgs boson production are also considered. 
Other contributions, such as W+jets or QCD multijet events with jets misidentified as leptons, are negligible.
Background simulation samples have been generated at NLO in QCD using powheg and MadGraph5 amc@nlo with FxFx merging and MadSpin. 
The signal samples of gluon fusion production of two Higgs bosons, and of spin-0 or spin-2 narrow resonances decaying into two Higgs bosons, have been generated at leading order (LO) in QCD using MadGraph5 amc@nlo version 2.2.2.0. 
The event generators used for both signal and background samples are interfaced with pythia 8.212.
The NNPDF 3.0 LO and NLO Parton Distribution Functions (PDF) are used.
Jets are reconstructed using a particle flow (PF) technique.
PF candidates are clustered to form jets using the anti-kT clustering algorithm with a distance parameter of 0.4.

Region of interest is defined as:
 - two leptons and two b-tagged jets
 - (Pt_l1, Pt_l2) &gt; (25GeV,15GeV) for the ee and mue channels 
 - (Pt_l1, Pt_l2) &gt; (20GeV,10GeV) for the mumu channel
 - (Pt_l1, Pt_l2) &gt; (25GeV,10GeV) for the emu channel
 - abs(eta_mu) &lt; 2.4
 - abs(eta_el) &lt; 2.5
 - pT_jet &gt; 20GeV
 - abs(eta_jet) &lt; 2.4
 - Delta_R(jet,lepton)&gt;0.3
 - 12 &lt; m_ll &lt; mZ −15 GeV
DOI: 10.17182/hepdata.83195.v1/t7
title: "Figure 5a" of "Search for resonant and nonresonant Higgs boson pair production in the bblnulnu final state in proton-proton collisions at sqrt(s) = 13 TeV"

description: The DNN output distributions in data and simulated events after requiring all selection criteria, in the e+e− channel. Output values towards 0 are background-like, while output values towards 1 are signal-like. The parameterised resonant DNN output is evaluated at mX=400GeV. The signal hypothesis has been scaled to a cross section of 5 pb for display purposes.
description: CERN-LHC. Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into lnulnu, through either W or Z bosons, and bbbar. Based on a sample of proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb−1.

The main background processes, in decreasing order of importance, are ttbar, Drell-Yan, and single top quark production. 
Diboson, triboson, ttV and SM single Higgs boson production are also considered. 
Other contributions, such as W+jets or QCD multijet events with jets misidentified as leptons, are negligible.
Background simulation samples have been generated at NLO in QCD using powheg and MadGraph5 amc@nlo with FxFx merging and MadSpin. 
The signal samples of gluon fusion production of two Higgs bosons, and of spin-0 or spin-2 narrow resonances decaying into two Higgs bosons, have been generated at leading order (LO) in QCD using MadGraph5 amc@nlo version 2.2.2.0. 
The event generators used for both signal and background samples are interfaced with pythia 8.212.
The NNPDF 3.0 LO and NLO Parton Distribution Functions (PDF) are used.
Jets are reconstructed using a particle flow (PF) technique.
PF candidates are clustered to form jets using the anti-kT clustering algorithm with a distance parameter of 0.4.

Region of interest is defined as:
 - two leptons and two b-tagged jets
 - (Pt_l1, Pt_l2) &gt; (25GeV,15GeV) for the ee and mue channels 
 - (Pt_l1, Pt_l2) &gt; (20GeV,10GeV) for the mumu channel
 - (Pt_l1, Pt_l2) &gt; (25GeV,10GeV) for the emu channel
 - abs(eta_mu) &lt; 2.4
 - abs(eta_el) &lt; 2.5
 - pT_jet &gt; 20GeV
 - abs(eta_jet) &lt; 2.4
 - Delta_R(jet,lepton)&gt;0.3
 - 12 &lt; m_ll &lt; mZ −15 GeV
DOI: 10.17182/hepdata.83195.v1/t8
title: "Figure 5b" of "Search for resonant and nonresonant Higgs boson pair production in the bblnulnu final state in proton-proton collisions at sqrt(s) = 13 TeV"

description: The DNN output distributions in data and simulated events after requiring all selection criteria, in the e+e− channel. Output values towards 0 are background-like, while output values towards 1 are signal-like. The parameterised nonresonant DNN output is evaluated at \kappa_\lambda=1, \kappa_t=1. The signal hypothesis has been scaled to a cross section of 5 pb for display purposes.
description: CERN-LHC. Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into lnulnu, through either W or Z bosons, and bbbar. Based on a sample of proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb−1.

The main background processes, in decreasing order of importance, are ttbar, Drell-Yan, and single top quark production. 
Diboson, triboson, ttV and SM single Higgs boson production are also considered. 
Other contributions, such as W+jets or QCD multijet events with jets misidentified as leptons, are negligible.
Background simulation samples have been generated at NLO in QCD using powheg and MadGraph5 amc@nlo with FxFx merging and MadSpin. 
The signal samples of gluon fusion production of two Higgs bosons, and of spin-0 or spin-2 narrow resonances decaying into two Higgs bosons, have been generated at leading order (LO) in QCD using MadGraph5 amc@nlo version 2.2.2.0. 
The event generators used for both signal and background samples are interfaced with pythia 8.212.
The NNPDF 3.0 LO and NLO Parton Distribution Functions (PDF) are used.
Jets are reconstructed using a particle flow (PF) technique.
PF candidates are clustered to form jets using the anti-kT clustering algorithm with a distance parameter of 0.4.

Region of interest is defined as:
 - two leptons and two b-tagged jets
 - (Pt_l1, Pt_l2) &gt; (25GeV,15GeV) for the ee and mue channels 
 - (Pt_l1, Pt_l2) &gt; (20GeV,10GeV) for the mumu channel
 - (Pt_l1, Pt_l2) &gt; (25GeV,10GeV) for the emu channel
 - abs(eta_mu) &lt; 2.4
 - abs(eta_el) &lt; 2.5
 - pT_jet &gt; 20GeV
 - abs(eta_jet) &lt; 2.4
 - Delta_R(jet,lepton)&gt;0.3
 - 12 &lt; m_ll &lt; mZ −15 GeV