{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.94800.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1805282"}},{"@id":"https://doi.org/10.1140/epjc/s10052-020-08677-2","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"Measurements of the Standard Model Higgs boson decaying into a $b\\bar{b}$ pair and produced in association with a $W$ or $Z$ boson decaying into leptons, using proton-proton collision data collected between 2015 and 2018 by the ATLAS detector, are presented. The measurements use data delivered by the Large Hadron Collider at a centre-of-mass energy of $\\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of 139 $fb^{-1}$. Cross-sections of associated production of a Higgs boson decaying into bottom quark pairs with an electroweak gauge boson, $W$ or $Z$, decaying into leptons are measured as a function of the gauge boson transverse momentum in kinematic fiducial volumes corresponding to the stage-1.2 simplified template cross-sections (STXS) scheme. Only the central kinematic region with an absolute rapidity of the Higgs boson $|y_{H}|$ of less than 2.5 is considered. The cross-section measurements are all consistent with the Standard Model expectations, and the total uncertainties vary from 30% in the high gauge boson transverse momentum regions to 85% in the low regions. Limits are subsequently set on the Wilson coefficients of a number of dim-6 operators in the Standard Model Effective Field Theory (SMEFT) which modify the $WH$ and $ZH$ processes as well as the Higgs boson decay to $b\\bar{b}$. These limits are also expressed in terms of constraints on an orthogonal set of linear combinations of operators to which this analysis is sensitive.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.94800.v2/t1","@type":"Dataset","description":"Best-fit values and uncertainties for $VH, V\\rightarrow\\mathrm{leptons}$ for the cross-section times the $H\\rightarrow b\\bar{b}$ branching fraction, in the reduced stage-1.2...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.94800.v2/t2","@type":"Dataset","description":"Observed correlations between the measured reduced stage-1.2 simplified template $VH, H \\rightarrow b\\bar{b}$ cross-sections (STXS), including both the statistical and...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.94800.v2/t3","@type":"Dataset","description":"Linear combination of Wilson coefficients corresponding to SMEFT operators in the Warsaw basis for which this analysis provides orthogonal constraints...","name":"Table 3"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1805282?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/94800"}],"inLanguage":"en","name":"Measurements of $WH$ and $ZH$ production in the $H \\rightarrow b\\bar{b}$ decay channel in $pp$ collisions at 13 TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1805282?version=2","version":2}