{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79407.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1628411"}},{"@id":"https://doi.org/10.1140/epjc/s10052-017-5491-4","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"A search for neutral heavy resonances is performed in the $WW\\to e\\nu\\mu\\nu$ decay channel using $pp$ collision data corresponding to an integrated luminosity of 36.1 fb$^{-1}$, collected at a centre-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. No evidence of such heavy resonances is found. In the search for production via the quark--antiquark annihilation or gluon--gluon fusion process, upper limits on $\\sigma_X \\times B(X \\to WW)$ as a function of the resonance mass are obtained in the mass range between 200 GeV and up to 5 TeV for various benchmark models: a Higgs-like scalar in different width scenarios, a two-Higgs-doublet model, a heavy vector triplet model, and a warped extra dimensions model. In the vector-boson fusion process, constraints are also obtained on these resonances, as well as on a Higgs boson in the Georgi--Machacek model and a heavy tensor particle coupling only to gauge bosons.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t1","@type":"Dataset","description":"Figure 1, left, subfigure a, Acceptance times efficiency as a function of signal mass for the ggF or qqA production....","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t2","@type":"Dataset","description":"Figure 1, right, subfigure b, Acceptance times efficiency as a function of signal mass for the VBF production. The \"0\"...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t3","@type":"Dataset","description":"Figure 2, left, subfigure a, Transverse mass distribution in the ggF top-quark control regions. For NWA signals, the \"0\" value...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t4","@type":"Dataset","description":"Figure 2, right, subfigure b, Transverse mass distribution in the VBF top-quark control regions. For NWA signals, the \"0\" value...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t5","@type":"Dataset","description":"Figure 3, left, subfigure a, Transverse mass distribution in the quasi-inclusive ggF WW control regions. The \"0\" value means lack...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t6","@type":"Dataset","description":"Figure 3, right, subfigure b, Transverse mass distribution in the quasi-inclusive VBF1Jet WW control regions. The \"0\" value means lack...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t7","@type":"Dataset","description":"Figure 4, top left, subfigure a, post-fit distributions of the transverse mass mT in the ggF Signal region. The \"0\"...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t8","@type":"Dataset","description":"Figure 4, top right, subfigure b, post-fit distributions of the transverse mass mT in the VBF1Jet Signal region. The \"0\"...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t9","@type":"Dataset","description":"Figure 4, bottom, subfigure c, post-fit distributions of the transverse mass mT in the VBF2Jet Signal region. The \"0\" value...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t10","@type":"Dataset","description":"Figure 5, left, subfigur a, Upper limits at 95% CL on the Higgs boson production cross section times branching fraction...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t11","@type":"Dataset","description":"Figure 5, right, subfigure b, Upper limits at 95% CL on the Higgs boson production cross section times branching fraction...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t12","@type":"Dataset","description":"Figure 6, Upper limits at 95% CL on the total ggF and VBF Higgs boson production cross section times branching...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t13","@type":"Dataset","description":"Figure 9, top left, subfigure a, Upper limits at 95% CL on the Higgs boson production cross section times branching...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t14","@type":"Dataset","description":"Figure 9, top right, subfigure b, Upper limits at 95% CL on the Higgs boson production cross section times branching...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t15","@type":"Dataset","description":"Figure 10, left, subfigure a, Upper limits at 95% CL on the resonance production cross section times branching fraction for...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t16","@type":"Dataset","description":"Figure 11, left, subfigure a, Upper limits at 95% CL on the resonance production cross section times branching fraction for...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t17","@type":"Dataset","description":"Figure 11, right, subfigure b, Upper limits at 95% CL on the resonance production cross section times branching fraction for...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t18","@type":"Dataset","description":"Figure 12, bottom, subfigure c, Upper limits at 95% CL on the resonance production cross section times branching fraction for...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t19","@type":"Dataset","description":"Figure 12, top right, subfigure b, Upper limits at 95% CL on the resonance production cross section times branching fraction...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t20","@type":"Dataset","description":"Figure 12, top left, subfigure a, Upper limits at 95% CL on the resonance production cross section times branching fraction...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t21","@type":"Dataset","description":"Auxiliary material Figure 2e, Event selection efficiencies in the VBF2J event categories as a function of the signal mass for...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t22","@type":"Dataset","description":"Auxiliary material Figure 2f, Event selection efficiencies in the VBF2J event categories for different kinds of VBF signals production. The...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t23","@type":"Dataset","description":"Auxiliary material Figure 2c, Event selection efficiencies in the VBF1J event categories as a function of the signal mass for...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t24","@type":"Dataset","description":"Auxiliary material Figure 2d, Event selection efficiencies in the VBF1J event categories for different kinds of VBF signals production. The...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t25","@type":"Dataset","description":"Auxiliary material Figure 2a, Event selection efficiencies in the ggF event categories as a function of the signal mass for...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t26","@type":"Dataset","description":"Auxiliary material Figure 2b, Event selection efficiencies in the ggF event categories for different kinds of VBF signals production. The...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t27","@type":"Dataset","description":"Auxiliary material Figure 6a, Upper limits at 95% CL on the Higgs production cross section times branching fraction in the...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t28","@type":"Dataset","description":"Auxiliary material Figure 6c, Upper limits at 95% CL on the Higgs production cross section times branching fraction in the...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t29","@type":"Dataset","description":"Auxiliary material Figure 6b, Upper limits at 95% CL on the Higgs production cross section times branching fraction in the...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t30","@type":"Dataset","description":"Auxiliary material Figure 6d, Upper limits at 95% CL on the Higgs production cross section times branching fraction in the...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t31","@type":"Dataset","description":"Auxiliary material Figure 7b, Upper limits at 95% CL on the total ggF and VBF Higgs production cross section times...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.79407.v1/t32","@type":"Dataset","description":"Auxiliary material Figure 7a, Upper limits at 95% CL on the total ggF and VBF Higgs production cross section times...","name":"Table 32"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1628411?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79407"}],"inLanguage":"en","name":"Search for heavy resonances decaying into $WW$ in the $e\\nu\\mu\\nu$ final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1628411?version=1","version":1}