{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.96390.v1/t5","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1821688"}},{"@id":"https://doi.org/10.1038/s41567-021-01225-z","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"The best-fit expected and observed distributions of the combined NN output in the SR for the $e\\tau$ channel for events...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1232801/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1232801/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1232801/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1232801/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1232801/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1821688?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/96390"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.96390.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1821688?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.96390.v1","@type":"Dataset","description":"A search for $Z$ boson decays into a $\\tau$ lepton and another lepton of different flavour ($\\ell$) with opposite electric charge is presented.\nThe data analysed correspond to $139\\text{ fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\\sqrt{s}=13\\text{ TeV}$ and $20.3\\text{ fb}^{-1}$ at $\\sqrt{s}=8\\text{ TeV}$, recorded with the ATLAS detector at the LHC.\n\nEvents are categorised according to the multiplicities and kinematics of reconstructed electrons, muons and $\\tau$ leptons, as well as the missing transverse momentum.\n\nThe signal region (SR) is defined by a $e^\\pm\\tau^\\mp$ or $\\mu^\\pm\\tau^\\mp$ final state with $m_\\mathrm{T}(\\tau_\\mathrm{had-vis}, E_\\mathrm{T}^\\mathrm{miss})&lt;35\\text{ GeV}$.\n\nThe same-sign validation region (VRSS) is defined similarly to the SR but with a $e^\\pm\\tau^\\pm$ or $\\mu^\\pm\\tau^\\pm$ final state.\n\nThe control region enhanced in $Z\\rightarrow\\tau\\tau$ events (CRZ$\\tau\\tau$) is defined similarly to the SR but with $m_\\mathrm{T}(\\tau_\\mathrm{had-vis}, E_\\mathrm{T}^\\mathrm{miss})&gt;35\\text{ GeV}$, $m_\\mathrm{T}(\\ell, E_\\mathrm{T}^\\mathrm{miss})&lt;40$ GeV and $70\\text{ GeV}&lt;m_\\mathrm{coll}(\\ell,\\tau)&lt;110\\text{ GeV}$, where $m_\\mathrm{coll}$ is the collinear mass.\n\nNeural network (NN) classifiers are used to discriminate between signal and background events. The combined NN output is fit to data in the SR and CRZ$\\tau\\tau$ to derive exclusion upper limits on the lepton-flavour-violating branching fraction $\\mathcal{B}(Z\\rightarrow\\ell\\tau)$.","name":"Search for charged-lepton-flavour violation in $Z$-boson decays with the ATLAS detector","url":"https://www.hepdata.net/record/ins1821688?version=1"},"keywords":"P P --> Z0 < E TAU >, 13000.0, Lepton Flavour Violation, LFV, Z decay","name":"Combined NN output distribution in SR, $e\\tau$ 1P","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/114814","version":1}