cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83179.v1/t19
title: "Table 19" of "Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% credibility-level upper limits on cross section times acceptance times branching ratio of X --&gt; bb, including kinematic acceptance and b-tagging efficiencies, for resonances exhibiting a generic Gaussian shape at particle level. The table shows the limits obtained from the inclusive b-jet selection. The limits corresponding to Gaussian-shaped resonances with width of Γ(X)/m(X) = 3%.
description: A search for new resonances decaying into jets containing b-hadrons in pp collisions with the ATLAS detector at the LHC is presented in the dijet mass range from 0.57 TeV to 7 TeV. The dataset corresponds to an integrated luminosity of up to 36.1 $fb^{−1}$ collected in 2015 and 2016 at √s=13 TeV. No evidence of a significant excess of events above the smooth background shape is found. Upper cross-section limits and lower limits on the corresponding signal mass parameters for several types of signal hypotheses are provided at 95% CL. In addition, 95% CL upper limits are set on the cross-sections for new processes that would produce Gaussian-shaped signals in the di-b-jet mass distributions.
DOI: 10.17182/hepdata.83179.v1/t20
title: "Table 20" of "Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% credibility-level upper limits on cross section times acceptance times branching ratio of X --&gt; bb, including kinematic acceptance and b-tagging efficiencies, for resonances exhibiting a generic Gaussian shape at particle level. The table shows the limits obtained from the inclusive b-jet selection. The limits corresponding to Gaussian-shaped resonances with width of Γ(X)/m(X) = 7%.
description: A search for new resonances decaying into jets containing b-hadrons in pp collisions with the ATLAS detector at the LHC is presented in the dijet mass range from 0.57 TeV to 7 TeV. The dataset corresponds to an integrated luminosity of up to 36.1 $fb^{−1}$ collected in 2015 and 2016 at √s=13 TeV. No evidence of a significant excess of events above the smooth background shape is found. Upper cross-section limits and lower limits on the corresponding signal mass parameters for several types of signal hypotheses are provided at 95% CL. In addition, 95% CL upper limits are set on the cross-sections for new processes that would produce Gaussian-shaped signals in the di-b-jet mass distributions.
DOI: 10.17182/hepdata.83179.v1/t21
title: "Table 21" of "Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% credibility-level upper limits on cross section times acceptance times branching ratio of X --&gt; bb, including kinematic acceptance and b-tagging efficiencies, for resonances exhibiting a generic Gaussian shape at particle level. The table shows the limits obtained from the inclusive b-jet selection. The limits corresponding to Gaussian-shaped resonances with width of Γ(X)/m(X) = 10%.
description: A search for new resonances decaying into jets containing b-hadrons in pp collisions with the ATLAS detector at the LHC is presented in the dijet mass range from 0.57 TeV to 7 TeV. The dataset corresponds to an integrated luminosity of up to 36.1 $fb^{−1}$ collected in 2015 and 2016 at √s=13 TeV. No evidence of a significant excess of events above the smooth background shape is found. Upper cross-section limits and lower limits on the corresponding signal mass parameters for several types of signal hypotheses are provided at 95% CL. In addition, 95% CL upper limits are set on the cross-sections for new processes that would produce Gaussian-shaped signals in the di-b-jet mass distributions.
DOI: 10.17182/hepdata.83179.v1/t22
title: "Table 22" of "Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% credibility-level upper limits on cross section times acceptance times branching ratio of X --&gt; bb, including kinematic acceptance and b-tagging efficiencies, for resonances exhibiting a generic Gaussian shape at particle level. The table shows the limits obtained from the inclusive b-jet selection. The limits corresponding to Gaussian-shaped resonances with width of Γ(X)/m(X) = 15%.
description: A search for new resonances decaying into jets containing b-hadrons in pp collisions with the ATLAS detector at the LHC is presented in the dijet mass range from 0.57 TeV to 7 TeV. The dataset corresponds to an integrated luminosity of up to 36.1 $fb^{−1}$ collected in 2015 and 2016 at √s=13 TeV. No evidence of a significant excess of events above the smooth background shape is found. Upper cross-section limits and lower limits on the corresponding signal mass parameters for several types of signal hypotheses are provided at 95% CL. In addition, 95% CL upper limits are set on the cross-sections for new processes that would produce Gaussian-shaped signals in the di-b-jet mass distributions.
DOI: 10.17182/hepdata.83179.v1/t23
title: "Table 23" of "Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% credibility-level upper limits on cross section times acceptance times branching ratio of X --&gt; bb, including kinematic acceptance and b-tagging efficiencies, for resonances exhibiting a generic Gaussian shape at particle level. The table shows the limits obtained from the combined low- and high-mass two b-tags selection. The limits corresponding to Gaussian-shaped resonances with width of Γ(X)/m(X) = 3%.
description: A search for new resonances decaying into jets containing b-hadrons in pp collisions with the ATLAS detector at the LHC is presented in the dijet mass range from 0.57 TeV to 7 TeV. The dataset corresponds to an integrated luminosity of up to 36.1 $fb^{−1}$ collected in 2015 and 2016 at √s=13 TeV. No evidence of a significant excess of events above the smooth background shape is found. Upper cross-section limits and lower limits on the corresponding signal mass parameters for several types of signal hypotheses are provided at 95% CL. In addition, 95% CL upper limits are set on the cross-sections for new processes that would produce Gaussian-shaped signals in the di-b-jet mass distributions.
DOI: 10.17182/hepdata.83179.v1/t24
title: "Table 24" of "Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% credibility-level upper limits on cross section times acceptance times branching ratio of X --&gt; bb, including kinematic acceptance and b-tagging efficiencies, for resonances exhibiting a generic Gaussian shape at particle level. The table shows the limits obtained from the combined low- and high-mass two b-tags selection. The limits corresponding to Gaussian-shaped resonances with width of Γ(X)/m(X) = 7%.
description: A search for new resonances decaying into jets containing b-hadrons in pp collisions with the ATLAS detector at the LHC is presented in the dijet mass range from 0.57 TeV to 7 TeV. The dataset corresponds to an integrated luminosity of up to 36.1 $fb^{−1}$ collected in 2015 and 2016 at √s=13 TeV. No evidence of a significant excess of events above the smooth background shape is found. Upper cross-section limits and lower limits on the corresponding signal mass parameters for several types of signal hypotheses are provided at 95% CL. In addition, 95% CL upper limits are set on the cross-sections for new processes that would produce Gaussian-shaped signals in the di-b-jet mass distributions.
DOI: 10.17182/hepdata.83179.v1/t25
title: "Table 25" of "Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% credibility-level upper limits on cross section times acceptance times branching ratio of X --&gt; bb, including kinematic acceptance and b-tagging efficiencies, for resonances exhibiting a generic Gaussian shape at particle level. The table shows the limits obtained from the combined low- and high-mass two b-tags selection. The limits corresponding to Gaussian-shaped resonances with width of Γ(X)/m(X) = 10%.
description: A search for new resonances decaying into jets containing b-hadrons in pp collisions with the ATLAS detector at the LHC is presented in the dijet mass range from 0.57 TeV to 7 TeV. The dataset corresponds to an integrated luminosity of up to 36.1 $fb^{−1}$ collected in 2015 and 2016 at √s=13 TeV. No evidence of a significant excess of events above the smooth background shape is found. Upper cross-section limits and lower limits on the corresponding signal mass parameters for several types of signal hypotheses are provided at 95% CL. In addition, 95% CL upper limits are set on the cross-sections for new processes that would produce Gaussian-shaped signals in the di-b-jet mass distributions.
DOI: 10.17182/hepdata.83179.v1/t26
title: "Table 26" of "Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% credibility-level upper limits on cross section times acceptance times branching ratio of X --&gt; bb, including kinematic acceptance and b-tagging efficiencies, for resonances exhibiting a generic Gaussian shape at particle level. The table shows the limits obtained from the combined low- and high-mass two b-tags selection. The limits corresponding to Gaussian-shaped resonances with width of Γ(X)/m(X) = 15%.
description: A search for new resonances decaying into jets containing b-hadrons in pp collisions with the ATLAS detector at the LHC is presented in the dijet mass range from 0.57 TeV to 7 TeV. The dataset corresponds to an integrated luminosity of up to 36.1 $fb^{−1}$ collected in 2015 and 2016 at √s=13 TeV. No evidence of a significant excess of events above the smooth background shape is found. Upper cross-section limits and lower limits on the corresponding signal mass parameters for several types of signal hypotheses are provided at 95% CL. In addition, 95% CL upper limits are set on the cross-sections for new processes that would produce Gaussian-shaped signals in the di-b-jet mass distributions.
DOI: 10.17182/hepdata.83180.v1/t1
title: "Table 1" of "Search for dark matter in events with a hadronically decaying vector boson and missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: The product of the acceptance and effifiency. Defined as the number of signal events satisfying the full set of selection criteria, divided by the total number of generated signal events, after the full event selection for the combined mono-W and mono-Z signal of the simplified vector-mediator model, shown in dependence on mass of the Z' mediator (mZp). For a given model, the signal contributions from each category are summed together.
description: CERN-LHC. This entry relates to the search for Dark Matter (DM) in association with a hadronically decaying vector boson with 36.1 fb-1 of pp collision data at a center-of-mass energy of sqrt(s) = 13 TeV recorded by the ATLAS detector at the LHC. In adition to hadronic decays of W and Z bosons, decays of the non-Standard-Model vector boson Z' of unknown masses are also considered for the first time (mono-Z'). The results are interpreted in terms of limits on the invisible Higgs boson decays into Dark Matter particles, constraints on the patamter space of the simplified vector-mediator model and generic upper limits on the visible detector-level cross sections for the W/Z+DM production. The results of the mono-Z' are shown in the frame of two simplified-model scenarios involving the DM production in assocaiation with the Z' boson. These are the dark Higgs model and the dark fermion model, each with a light and heavy dark sector scenario. 

The final states considered are missing transverse momentum in association with two well-separated jets or one large-radius jet from a highly boosted vector boson. These are referred to as the resolved and merged topologies respectivaly. 

The resolved topology is defined as : 

- MET &gt; 150 GeV
- &gt;= 2j, 0l
- &lt;= 2 b-tagged small-R jets
- dPhi(MET, jj) &gt;120deg
- min dPhi[MET, j_i] &gt;20deg
- pTmiss &gt; 30 GeV or &gt;= 2 b-tagged jets
- dPhi(MET, pTmiss) &lt; 90deg
- pT(j1) &gt; 45 GeV
- sum of jet pT &gt; 120 (150) GeV for 2 (&gt;= 3jets)

if 0 b-tagged jets and mZ' &lt; 200GeV : 
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV
if 0 b-tagged jets and mZ' &gt;= 200GeV : 
- [0.85*mZ' &lt; mjj &lt; mZ'+20] GeV
if 1/2 b-tagged jets and mZ' &lt; 200GeV : 
- [0.75*mZ' &lt; mjj &lt; mZ'+10] GeV
if 1/2 b-tagged jets and mZ' &gt;= 200GeV : 
- [0.80*mZ' &lt; mjj &lt; mZ'+20] GeV

The merged topology is defined as : 
- MET &gt; 250 GeV
- &gt;= 1J, 0l
- no b-tagged jets outside of J
- dPhi(MET, J) &gt;120deg
- min dPhi[MET, j_i] &gt;20deg
- pTmiss &gt; 30 GeV or &gt;= 2 b-tagged jets
- dPhi(MET, pTmiss) &lt; 90deg

if 0 b-tagged jets and mZ' &lt; 100GeV :
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV
if 1/2 b-tagged jets and mZ' &lt; 100GeV :
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV

mZ' &gt; 100GeV :
- no merged selection
DOI: 10.17182/hepdata.83180.v1/t2
title: "Table 2" of "Search for dark matter in events with a hadronically decaying vector boson and missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: The product of the acceptance and effifiency. Defined as the number of signal events satisfying the full set of selection criteria, divided by the total number of generated signal events, after the full event selection for the mono-Z' dark fermion and dark-Higgs signal models, shown in dependence on the mass of the Z' mediator (mZp). For a given model, the signal contributions from each category are summed together.
description: CERN-LHC. This entry relates to the search for Dark Matter (DM) in association with a hadronically decaying vector boson with 36.1 fb-1 of pp collision data at a center-of-mass energy of sqrt(s) = 13 TeV recorded by the ATLAS detector at the LHC. In adition to hadronic decays of W and Z bosons, decays of the non-Standard-Model vector boson Z' of unknown masses are also considered for the first time (mono-Z'). The results are interpreted in terms of limits on the invisible Higgs boson decays into Dark Matter particles, constraints on the patamter space of the simplified vector-mediator model and generic upper limits on the visible detector-level cross sections for the W/Z+DM production. The results of the mono-Z' are shown in the frame of two simplified-model scenarios involving the DM production in assocaiation with the Z' boson. These are the dark Higgs model and the dark fermion model, each with a light and heavy dark sector scenario. 

The final states considered are missing transverse momentum in association with two well-separated jets or one large-radius jet from a highly boosted vector boson. These are referred to as the resolved and merged topologies respectivaly. 

The resolved topology is defined as : 

- MET &gt; 150 GeV
- &gt;= 2j, 0l
- &lt;= 2 b-tagged small-R jets
- dPhi(MET, jj) &gt;120deg
- min dPhi[MET, j_i] &gt;20deg
- pTmiss &gt; 30 GeV or &gt;= 2 b-tagged jets
- dPhi(MET, pTmiss) &lt; 90deg
- pT(j1) &gt; 45 GeV
- sum of jet pT &gt; 120 (150) GeV for 2 (&gt;= 3jets)

if 0 b-tagged jets and mZ' &lt; 200GeV : 
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV
if 0 b-tagged jets and mZ' &gt;= 200GeV : 
- [0.85*mZ' &lt; mjj &lt; mZ'+20] GeV
if 1/2 b-tagged jets and mZ' &lt; 200GeV : 
- [0.75*mZ' &lt; mjj &lt; mZ'+10] GeV
if 1/2 b-tagged jets and mZ' &gt;= 200GeV : 
- [0.80*mZ' &lt; mjj &lt; mZ'+20] GeV

The merged topology is defined as : 
- MET &gt; 250 GeV
- &gt;= 1J, 0l
- no b-tagged jets outside of J
- dPhi(MET, J) &gt;120deg
- min dPhi[MET, j_i] &gt;20deg
- pTmiss &gt; 30 GeV or &gt;= 2 b-tagged jets
- dPhi(MET, pTmiss) &lt; 90deg

if 0 b-tagged jets and mZ' &lt; 100GeV :
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV
if 1/2 b-tagged jets and mZ' &lt; 100GeV :
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV

mZ' &gt; 100GeV :
- no merged selection
DOI: 10.17182/hepdata.83180.v1/t3
title: "Table 3" of "Search for dark matter in events with a hadronically decaying vector boson and missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the merged event topology after the profile-likelihood fit. This is shown for the 0b-tagged jet, high purity, event category.
description: CERN-LHC. This entry relates to the search for Dark Matter (DM) in association with a hadronically decaying vector boson with 36.1 fb-1 of pp collision data at a center-of-mass energy of sqrt(s) = 13 TeV recorded by the ATLAS detector at the LHC. In adition to hadronic decays of W and Z bosons, decays of the non-Standard-Model vector boson Z' of unknown masses are also considered for the first time (mono-Z'). The results are interpreted in terms of limits on the invisible Higgs boson decays into Dark Matter particles, constraints on the patamter space of the simplified vector-mediator model and generic upper limits on the visible detector-level cross sections for the W/Z+DM production. The results of the mono-Z' are shown in the frame of two simplified-model scenarios involving the DM production in assocaiation with the Z' boson. These are the dark Higgs model and the dark fermion model, each with a light and heavy dark sector scenario. 

The final states considered are missing transverse momentum in association with two well-separated jets or one large-radius jet from a highly boosted vector boson. These are referred to as the resolved and merged topologies respectivaly. 

The resolved topology is defined as : 

- MET &gt; 150 GeV
- &gt;= 2j, 0l
- &lt;= 2 b-tagged small-R jets
- dPhi(MET, jj) &gt;120deg
- min dPhi[MET, j_i] &gt;20deg
- pTmiss &gt; 30 GeV or &gt;= 2 b-tagged jets
- dPhi(MET, pTmiss) &lt; 90deg
- pT(j1) &gt; 45 GeV
- sum of jet pT &gt; 120 (150) GeV for 2 (&gt;= 3jets)

if 0 b-tagged jets and mZ' &lt; 200GeV : 
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV
if 0 b-tagged jets and mZ' &gt;= 200GeV : 
- [0.85*mZ' &lt; mjj &lt; mZ'+20] GeV
if 1/2 b-tagged jets and mZ' &lt; 200GeV : 
- [0.75*mZ' &lt; mjj &lt; mZ'+10] GeV
if 1/2 b-tagged jets and mZ' &gt;= 200GeV : 
- [0.80*mZ' &lt; mjj &lt; mZ'+20] GeV

The merged topology is defined as : 
- MET &gt; 250 GeV
- &gt;= 1J, 0l
- no b-tagged jets outside of J
- dPhi(MET, J) &gt;120deg
- min dPhi[MET, j_i] &gt;20deg
- pTmiss &gt; 30 GeV or &gt;= 2 b-tagged jets
- dPhi(MET, pTmiss) &lt; 90deg

if 0 b-tagged jets and mZ' &lt; 100GeV :
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV
if 1/2 b-tagged jets and mZ' &lt; 100GeV :
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV

mZ' &gt; 100GeV :
- no merged selection
DOI: 10.17182/hepdata.83180.v1/t4
title: "Table 4" of "Search for dark matter in events with a hadronically decaying vector boson and missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the merged event topology after the profile-likelihood fit. This is shown for the 0b-tagged jet, low purity, event category.
description: CERN-LHC. This entry relates to the search for Dark Matter (DM) in association with a hadronically decaying vector boson with 36.1 fb-1 of pp collision data at a center-of-mass energy of sqrt(s) = 13 TeV recorded by the ATLAS detector at the LHC. In adition to hadronic decays of W and Z bosons, decays of the non-Standard-Model vector boson Z' of unknown masses are also considered for the first time (mono-Z'). The results are interpreted in terms of limits on the invisible Higgs boson decays into Dark Matter particles, constraints on the patamter space of the simplified vector-mediator model and generic upper limits on the visible detector-level cross sections for the W/Z+DM production. The results of the mono-Z' are shown in the frame of two simplified-model scenarios involving the DM production in assocaiation with the Z' boson. These are the dark Higgs model and the dark fermion model, each with a light and heavy dark sector scenario. 

The final states considered are missing transverse momentum in association with two well-separated jets or one large-radius jet from a highly boosted vector boson. These are referred to as the resolved and merged topologies respectivaly. 

The resolved topology is defined as : 

- MET &gt; 150 GeV
- &gt;= 2j, 0l
- &lt;= 2 b-tagged small-R jets
- dPhi(MET, jj) &gt;120deg
- min dPhi[MET, j_i] &gt;20deg
- pTmiss &gt; 30 GeV or &gt;= 2 b-tagged jets
- dPhi(MET, pTmiss) &lt; 90deg
- pT(j1) &gt; 45 GeV
- sum of jet pT &gt; 120 (150) GeV for 2 (&gt;= 3jets)

if 0 b-tagged jets and mZ' &lt; 200GeV : 
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV
if 0 b-tagged jets and mZ' &gt;= 200GeV : 
- [0.85*mZ' &lt; mjj &lt; mZ'+20] GeV
if 1/2 b-tagged jets and mZ' &lt; 200GeV : 
- [0.75*mZ' &lt; mjj &lt; mZ'+10] GeV
if 1/2 b-tagged jets and mZ' &gt;= 200GeV : 
- [0.80*mZ' &lt; mjj &lt; mZ'+20] GeV

The merged topology is defined as : 
- MET &gt; 250 GeV
- &gt;= 1J, 0l
- no b-tagged jets outside of J
- dPhi(MET, J) &gt;120deg
- min dPhi[MET, j_i] &gt;20deg
- pTmiss &gt; 30 GeV or &gt;= 2 b-tagged jets
- dPhi(MET, pTmiss) &lt; 90deg

if 0 b-tagged jets and mZ' &lt; 100GeV :
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV
if 1/2 b-tagged jets and mZ' &lt; 100GeV :
- [0.85*mZ' &lt; mjj &lt; mZ'+10] GeV

mZ' &gt; 100GeV :
- no merged selection