{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.85867.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1645246"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-6049-9","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"CERN-LHC. A measurement of the electroweak (EW) production of two jets in association with a   Z  boson in proton-proton collisions at  $\\sqrt{s}$=13TeV. The cross section is measured in a kinematic region defined by invariant masses $m_{ll}~&gt;~50$ GeV, $m_{jj}~&gt;~120$ GeV, and transverse momenta $p_{Tj}~&gt;~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction. The measurement is based on data recorded in 2016 by the CMS experiment at the LHC corresponding to an integrated luminosity of 35.9 $fb^{-1}$. Limits on anomalous trilinear gauge couplings associated with dimension-six operators are given in the framework of an effective field theory and an effective Lagrangian.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t1","@type":"Dataset","description":"One-dimensional limits on the ATGC EFT parameters at 95% CL","name":"Limits on the ATGC EFT parameters"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t2","@type":"Dataset","description":"One-dimensional limits on the ATGC effective Lagrangian (LEP parametrization) parameters at 95% CL","name":"Limits on the ATGC effective Lagrangian"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t3","@type":"Dataset","description":"The best fit signal strength for dielectron, dimuon and combined dilepton channels. The measurement is performed in a kinematic region...","name":"Best fit signal strength"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t4","@type":"Dataset","description":"Measured signal cross section for dielectron, dimuon and combined dilepton channels. The measurement is performed in a kinematic region defined...","name":"Measured signal cross section"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t5","@type":"Dataset","description":"Distributions of $p_{TZ}$ in data and total SM background, EW Zjj signal and two ATGC scenarios in the dimuon channel","name":"pT of the Z boson, dimuon"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t6","@type":"Dataset","description":"Distributions of $p_{TZ}$ in data and total SM background, EW Zjj signal and two ATGC scenarios in the dielectron channel","name":"pT of the Z boson, dielectron"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t7","@type":"Dataset","description":"Distributions of $m_{jj}$ in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is...","name":"mjj of the Z boson, dimuon"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t8","@type":"Dataset","description":"Distributions of $m_{jj}$ in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is...","name":"mjj of the Z boson, dielectron"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t9","@type":"Dataset","description":"Distributions of the transformed BDT discriminant in data and total SM background and EW Zjj signal in the dimuon channel....","name":"Transformed BDT, dimuon"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t10","@type":"Dataset","description":"Distributions of the transformed BDT discriminant in data and total SM background and EW Zjj signal in the dimuon channel....","name":"Transformed BDT, dielectron"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t11","@type":"Dataset","description":"Efficiency of a gap activity veto in dielectron and dimuon events with BDT &gt; 0.92, as a function of the...","name":"Veto efficiency, Third jet $p_T$"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t12","@type":"Dataset","description":"Efficiency of a gap activity veto in dielectron and dimuon events with BDT &gt; 0.92, as a function of total...","name":"Veto efficiency, $H_T$"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t13","@type":"Dataset","description":"Efficiency of a gap activity veto in dielectron and dimuon events with BDT &gt; 0.92, as a function of total...","name":"Veto efficiency, Soft $H_T$"},{"@id":"https://doi.org/10.17182/hepdata.85867.v1/t14","@type":"Dataset","description":"Efficiency of a gap activity veto in dielectron and dimuon events with BDT &gt; 0.92, as a function of the...","name":"Veto efficiency, leading soft jet $p_T$"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1645246?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/85867"}],"inLanguage":"en","name":"Electroweak production of two jets in association with a Z boson in proton-proton collisions at $\\sqrt{s}= $ 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1645246?version=1","version":1}
