{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83180.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1684341"}},{"@id":"https://doi.org/10.1007/JHEP10(2018)180","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","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. \n\nThe 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. \n\nThe resolved topology is defined as : \n\n- MET > 150 GeV\n- >= 2j, 0l\n- <= 2 b-tagged small-R jets\n- dPhi(MET, jj) >120deg\n- min dPhi[MET, j_i] >20deg\n- pTmiss > 30 GeV or >= 2 b-tagged jets\n- dPhi(MET, pTmiss) < 90deg\n- pT(j1) > 45 GeV\n- sum of jet pT > 120 (150) GeV for 2 (>= 3jets)\n\nif 0 b-tagged jets and mZ' < 200GeV : \n- [0.85*mZ' < mjj < mZ'+10] GeV\nif 0 b-tagged jets and mZ' >= 200GeV : \t\n- [0.85*mZ' < mjj < mZ'+20] GeV\nif 1/2 b-tagged jets and mZ' < 200GeV : \n- [0.75*mZ' < mjj < mZ'+10] GeV\nif 1/2 b-tagged jets and mZ' >= 200GeV : \n- [0.80*mZ' < mjj < mZ'+20] GeV\n\nThe merged topology is defined as : \n- MET > 250 GeV\n- >= 1J, 0l\n- no b-tagged jets outside of J\n- dPhi(MET, J) >120deg\n- min dPhi[MET, j_i] >20deg\n- pTmiss > 30 GeV or >= 2 b-tagged jets\n- dPhi(MET, pTmiss) < 90deg\n\nif 0 b-tagged jets and mZ' < 100GeV :\n- [0.85*mZ' < mjj < mZ'+10] GeV\nif 1/2 b-tagged jets and mZ' < 100GeV :\n- [0.85*mZ' < mjj < mZ'+10] GeV\n\nmZ' > 100GeV :\n- no merged selection","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t1","@type":"Dataset","description":"The product of the acceptance and effifiency. Defined as the number of signal events satisfying the full set of selection...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t2","@type":"Dataset","description":"The product of the acceptance and effifiency. Defined as the number of signal events satisfying the full set of selection...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t3","@type":"Dataset","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...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t4","@type":"Dataset","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...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t5","@type":"Dataset","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...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t6","@type":"Dataset","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...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t7","@type":"Dataset","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...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t8","@type":"Dataset","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...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t9","@type":"Dataset","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...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t10","@type":"Dataset","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...","name":"Table 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18"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t19","@type":"Dataset","description":"The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t20","@type":"Dataset","description":"The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t21","@type":"Dataset","description":"The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t22","@type":"Dataset","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...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t23","@type":"Dataset","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...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t24","@type":"Dataset","description":"Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t25","@type":"Dataset","description":"Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t26","@type":"Dataset","description":"Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t27","@type":"Dataset","description":"Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t28","@type":"Dataset","description":"Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp),...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t29","@type":"Dataset","description":"Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp),...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t30","@type":"Dataset","description":"Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp),...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t31","@type":"Dataset","description":"Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp),...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t32","@type":"Dataset","description":"The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t33","@type":"Dataset","description":"The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t34","@type":"Dataset","description":"The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.83180.v1/t35","@type":"Dataset","description":"The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region...","name":"Table 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