{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.65524.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1308524"}},{"@id":"https://doi.org/10.1007/JHEP09(2014)037","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2014","description":"CERN-LHC. This paper presents a search for new particles in events with one lepton (electron or muon) and missing transverse momentum using 20.3 fb-1 of proton-proton collision data at sqrt(s)=8 TeV recorded by the ATLAS experiment at the Large Hadron Collider. No significant excess beyond Standard Model expectations is observed. A WPRIME with Sequential Standard Model couplings is excluded at the 95% confidence level for masses up to 3.24 TeV. Excited chiral bosons (W*) with equivalent coupling strengths are excluded for masses up to 3.21 TeV. In the framework of an effective field theory limits are also set on the dark matter-nucleon scattering cross-section as well as the mass scale M* of the unknown mediating interaction for dark matter pair production in association with a leptonically decaying W.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t1","@type":"Dataset","description":"Spectrum of lepton PT for the electron channel after the event selection. The spectrum is shown with the requirement MT...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t2","@type":"Dataset","description":"Spectrum of lepton PT for the muon channel after the event selection. The spectrum is shown with the requirement MT...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t3","@type":"Dataset","description":"Spectrum of ETmiss for the electron channel after the event selection. The spectrum is shown with the requirement MT >...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t4","@type":"Dataset","description":"Spectrum of ETmiss for the muon channel after the event selection. The spectrum is shown with the requirement MT >...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t5","@type":"Dataset","description":"Spectrum of MT for the electron channel after the event selection.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t6","@type":"Dataset","description":"Spectrum of MT for the muon channel after the event selection.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t7","@type":"Dataset","description":"Observed and expected limits on SIGMA*B for WPRIME at 95% CL in the electron channel.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t8","@type":"Dataset","description":"Observed and expected limits on SIGMA*B for W* at 95% CL in the electron channel.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t9","@type":"Dataset","description":"Observed and expected limits on SIGMA*B for WPRIME at 95% CL in the muon channel.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t10","@type":"Dataset","description":"Observed and expected limits on SIGMA*B for W* at 95% CL in the muon channel.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t11","@type":"Dataset","description":"Observed and expected limits on SIGMA*B for WPRIME at 95% CL for the combination of the electron and muon channels.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t12","@type":"Dataset","description":"Observed and expected limits on SIGMA*B for W* at 95% CL for the combination of the electron and muon channels.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t13","@type":"Dataset","description":"Observed limits on M* as a function of the DM particle mass M(chi) at 90% CL for the combination of...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t14","@type":"Dataset","description":"Observed limits on the DM-nucleon scattering cross-section as a function of M(chi) at 90% CL for various operators in the...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t15","@type":"Dataset","description":"Observed limits on M* as a function of the DM particle mass M(chi) at 90% CL in the electron for...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t16","@type":"Dataset","description":"Observed limits on M* as a function of the DM particle mass M(chi) at 90% CL in the muon for...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t17","@type":"Dataset","description":"Observed limits on M* as a function of the DM particle mass M(chi) at 95% CL in the electron for...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t18","@type":"Dataset","description":"Observed limits on M* as a function of the DM particle mass M(chi) at 95% CL in the muon for...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.65524.v1/t19","@type":"Dataset","description":"Observed limits on M* as a function of the DM particle mass M(chi) at 95% CL for the combination of...","name":"Table 19"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1308524?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/65524"}],"inLanguage":"en","name":"Search for new particles in events with one lepton and missing transverse momentum in $pp$ collisions at $\\sqrt{s}$ = 8 TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1308524?version=1","version":1}