{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83539.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1684645"}},{"@id":"https://doi.org/10.1103/PhysRevLett.121.191801","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"CERN-ATLAS. Searches for resonant and non-resonant Higgs boson pair-production in the bb tau tau decay channel in pp collisions at sqrt(s)=13 TeV with the ATLAS detector","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t1","@type":"Dataset","description":"Observed and expected limits at 95% CL on the cross-sections of RS Graviton to HH for k/MPl = 1 process","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t2","@type":"Dataset","description":"Observed and expected limits at 95% CL on the cross-sections of RS Graviton to HH for k/MPl = 2 process","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t3","@type":"Dataset","description":"Observed and expected limits at 95% CL on the cross-sections of hMSSM scalar X to HH process","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t4","@type":"Dataset","description":"Acceptance x efficiency versus resonance mass for both lephad and hadhad channels in the RS bulk model with k/MPl =...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t5","@type":"Dataset","description":"Acceptance x efficiency versus resonance mass for both lephad and hadhad channels in the RS bulk model with k/MPl =...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t6","@type":"Dataset","description":"Acceptance x efficiency versus resonance mass for both lephad and hadhad channels in the scalar model","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t7","@type":"Dataset","description":"Upper limits on the production cross-section times the HH to bbtautau branching ratio for non-resonant HH at 95% CLS and...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t8","@type":"Dataset","description":"Upper limits on the production cross-section times the HH to bbtautau branching ratio divided by the SM prediction for non-resonant...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t9","@type":"Dataset","description":"Post-fit expected number of signal and background events and observed number of data events after applying the selection criteria and...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.83539.v1/t10","@type":"Dataset","description":"Post-fit expected number of signal and background events and observed number of data events in the last two bins of...","name":"Table 10"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1684645?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/83539"}],"inLanguage":"en","name":"A search for resonant and non-resonant Higgs boson pair production in the ${b\\bar{b}\\tau^+\\tau^-}$ decay channel 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/ins1684645?version=1","version":1}