cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83180.v1/t21
title: "Table 21" 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-Z' signal region with the resolved event topology for a Z' mass of 350 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, 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/t22
title: "Table 22" 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: Expected exclusion contours at 95% C.L. of the dark matter mediator particles (m_chi, m_Zp) for the combined mono-W and mono-Z search in the frame of the simplified model with the Dirac DM particles and couplings g_SM = 0.25 and g_DM = 1.
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/t23
title: "Table 23" 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: Observed exclusion contours at 95% C.L. of the dark matter mediator particles (m_chi, m_Zp) for the combined mono-W and mono-Z search in the frame of the simplified model with the Dirac DM particles and couplings g_SM = 0.25 and g_DM = 1.
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/t24
title: "Table 24" 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: Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark fermion model, with the light dark sector scenario, with parameters g_SM = 0.1 and g_DM = 1.
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/t25
title: "Table 25" 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: Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark fermion model, with the heavy dark sector scenario, with parameters g_SM = 0.1 and g_DM = 1.
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/t26
title: "Table 26" 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: Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark Higgs model, with the light dark sector scenario, with parameters g_SM = 0.1 and g_DM = 1.
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/t27
title: "Table 27" 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: Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark Higgs model, with the heavy dark sector scenario, with parameters g_SM = 0.1 and g_DM = 1.
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/t28
title: "Table 28" 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: Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp), for the mono-Z' dark fermion model, with the light dark sector scenario, with parameter g_DM = 1.
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