{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83785.v1/t11","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1711223"}},{"@id":"https://doi.org/10.1016/j.physletb.2019.05.012","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"Correlation matrix for the unfolded fiducial cross-section.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/420920/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/420920/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/420920/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/420920/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/420920/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1711223?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/83785"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.83785.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1711223?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.83785.v1","@type":"Dataset","description":"CERN-LHC.  An observation of electroweak $W^{\\pm}Z$ production in association with two jets in proton-proton collisions is presented. \nThe data collected by the ATLAS detector at the Large Hadron Collider in 2015 and 2016 at a centre-of-energy of $\\sqrt{s}$ = 13TeV are used, corresponding to an integrated luminosity of 36.1 $fb^{-1}$. \nEvents containing three identified leptons, either electrons or muons, and two jets are selected. \nThe electroweak production of $W^{\\pm}Z$ bosons in association with two jets is measured with an observed significance of 5.3 standard deviations. \nA fiducial cross section for electroweak production including interference effects is measured to be $\\sigma_{WZjj-EW}$ = 0.57^{+0.14}_{-0.13} (stat.) ^{+0.07}_{-0.06} (syst.) fb. \nDifferential cross section of $W^{\\pm}Zjj$ production for several kinematic observables are also measured.\n\nFiducial phase space definition for the measurement:\n- $p_{\\mathrm{T}}$ of electrons and muons from Z0 decays > 15 GeV\n- $p_{\\mathrm{T}}$ of electrons and muons from the $W^{\\pm}$ decays > 20 GeV\n- $|\\eta|$ of muons and electrons < 2.5\n- Leptons from the Z0 boson are separated by $\\Delta R(\\ell,\\ell) > 0.2$ from each other\n- Leptons from the Z0 and W bosons are separated by $\\Delta R(\\ell,\\ell) > 0.3$ from each other\n- |dilepton mass - Z0 mass| < 10 GeV\n- $m_{\\mathrm{T}}$ of $W^{\\pm}$ > 30 GeV.\n \n- at least 2 jets with opposite $|\\eta|$. Jets are particle level jets with anti-kt R=0.4.\n- $p_{\\mathrm{T}}$ of the two jets > 40 GeV\n- $|\\eta|$ of the two jets < 4.5\n- the first jet is chosen as the leading $p_{\\mathrm{T}}$ jet\n- the second jet is chosen among the remaining jets as the jet of highest $p_{\\mathrm{T}}$ with  $|\\eta|$ opposite to the first jets\n- invariant mass of the two jets > 500 GeV\n- leptons and jets separated by $\\Delta R(\\ell,jet) > 0.3$\n- processes with a b-quark in the initial state are excluded\n\n\n\nAt particle level, the kinematics of final-state prompt electrons and muons is computed including the contributions from\nfinal-state radiated photons within a distance in the ($\\eta,\\phi$) plane of $\\Delta R = \\sqrt{(\\Delta\\eta)^2 + (\\Delta\\phi)^2} = 0.1$ around the direction of the charged lepton.\nThese dressed leptons and the final-state neutrinos that do not originate from hadron or $\\tau$ decays  are associated with the $W$ and $Z$ boson decay products with an\nalgorithmic approach, called ``resonant shape''.\nThis algorithm is  based on the value of an estimator expressing\n   the product of the nominal line shapes of the $W$ and $Z$ resonances\n\n   $P = \\left| \\frac{1}{ m^2_{(\\ell^+,\\ell^-)} - \\left(m_Z^{\\textrm{PDG}}\\right)^2 + i \\; \\Gamma_Z^{\\textrm{PDG}} \\; m_Z^{\\textrm{PDG}} } \\right|^2  \\times \\; \\left| \\frac {1} { m^2_{(\\ell',\\nu_{\\ell'})} - \\left(m_W^{\\textrm{PDG}}\\right)^2 + i \\; \\Gamma_W^{\\textrm{PDG}} \\; m_W^{\\textrm{PDG}} } \\right|^2$\n\nwhere $m_Z^{\\textrm{PDG}}$ ($m_W^{\\textrm{PDG}}$) and $\\Gamma_Z^{\\textrm{PDG}}$ ($\\Gamma_W^{\\textrm{PDG}}$) are the world average mass and total width of the $Z$ ($W$) boson, respectively, as reported by the Particle Data Group \\cite{Agashe:2014kda}.\nThe input to the estimator is the invariant mass $m$ of all possible pairs ($\\ell^+,\\ell^-$) and ($\\ell',\\nu_{\\ell'}$)\nsatisfying the fiducial selection requirements defined in the next paragraph.\nThe final choice of which leptons are assigned to the $W$ or $Z$ bosons corresponds to the configuration  exhibiting the highest  value of the estimator.","name":"Observation of electroweak $W^{\\pm}Z$ boson pair production in association with two jets in $pp$ collisions at $\\sqrt{s} =$ 13 TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins1711223?version=1"},"keywords":"P P --> (W+ + W-) Z0 j j X, DSIG/DELTAPHIWZ, 13000.0","name":"Table 11","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/90460","version":1}