cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83195.v1/t9
title: "Figure 5c" 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^{+/-}mu^{-/+} 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/t10
title: "Figure 5d" 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^{+/-}mu^{-/+} 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
DOI: 10.17182/hepdata.83195.v1/t11
title: "Figure 5e" 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 mu+mu− 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/t12
title: "Figure 5f" 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 mu+mu− 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
DOI: 10.17182/hepdata.83195.v1/t13
title: "Figure 6a" 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, for the e+e- channel, in three different mjj regions. 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/t14
title: "Figure 6b" 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, for the e+e- channel, in three different mjj regions. 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
DOI: 10.17182/hepdata.83195.v1/t15
title: "Figure 6c" 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, for the e^{+/-}mu^{-/+} channel, in three different mjj regions. 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/t16
title: "Figure 6d" 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, for the e^{+/-}mu^{-/+} channel, in three different mjj regions. 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
DOI: 10.17182/hepdata.83195.v1/t17
title: "Figure 6e" 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, for the mu+mu- channel, in three different mjj regions. 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/t18
title: "Figure 6f" 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, for the mu+mu- channel, in three different mjj regions. 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