{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.94181.v3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1794169"}},{"@id":"https://doi.org/10.1016/j.physletb.2020.135710","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"Measurements of production cross sections of WZ and same-sign $W^\\pm W^\\pm$ boson pairs in association with two jets in proton-proton collisions at $\\sqrt{s}$=13TeV at the LHC are reported. The data sample corresponds to an integrated luminosity of 137$fb^{-1}$, collected with the CMS detector during 2016--2018. The measurements are performed in the leptonic decay modes $W^\\pm Z \\to \\ell^\\pm\\nu\\ell'^\\pm\\ell'^\\mp$ and $W^\\pm W^\\pm \\to \\ell^\\pm\\nu\\ell'^\\pm\\nu$, where $\\ell, \\ell' = e$, $\\mu$. Differential fiducial cross sections as functions of the invariant masses of the jet and charged lepton pairs, as well as of the leading-lepton transverse momentum, are measured for WW production and are consistent with the standard model predictions. The dependence of differential cross sections on the invariant mass of the jet pair is also measured for WZ production. An observation of electroweak production of WZ boson pairs is reported with an observed (expected) significance of 6.8 (5.3) standard deviations. Constraints are obtained on the structure of quartic vector boson interactions in the framework of effective field theory.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t1","@type":"Dataset","description":"Relative systematic uncertainties in the EW $W^\\pm W^\\pm$ and WZ cross section measurements in units of percent.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t2","@type":"Dataset","description":"Expected and observed yields from the standard model processeses in the WW signal region. The combination of the statistical and...","name":"Table 4a"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t3","@type":"Dataset","description":"Expected and observed yields from the standard model processeses in the WZ signal region. The combination of the statistical and...","name":"Table 4b"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t4","@type":"Dataset","description":"The measured inclusive fiducial cross section measurements. The WW fiducial region is defined by requiring two same-sign leptons with $p_{T}>20$,...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t5","@type":"Dataset","description":"Distributions of $m_{jj}$ in the WW signal region.","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t6","@type":"Dataset","description":"Distributions of $m_{ll}$ in the WW signal region.","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t7","@type":"Dataset","description":"Distributions of $m_{jj}$ in the WZ signal region.","name":"Figure 3c"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t8","@type":"Dataset","description":"Distributions of BDT score in the WZ signal region.","name":"Figure 3d"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t9","@type":"Dataset","description":"Absolute WW cross section in $m_{jj}$ bins.","name":"Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t10","@type":"Dataset","description":"Normalized WW cross section in $m_{jj}$ bins.","name":"Figure 4b"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t11","@type":"Dataset","description":"Absolute WW cross section in $m_{ll}$ bins.","name":"Figure 4c"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t12","@type":"Dataset","description":"Normalized WW cross section in $m_{ll}$ bins.","name":"Figure 4d"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t13","@type":"Dataset","description":"Absolute WW cross section in $p_{T}^{l max}$ bins.","name":"Figure 4e"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t14","@type":"Dataset","description":"Normalized WW cross section in $p_{T}^{l max}$ bins.","name":"Figure 4f"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t15","@type":"Dataset","description":"Absolute WZ cross section in $m_{jj}$ bins.","name":"Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t16","@type":"Dataset","description":"Normalized WZ cross section in $m_{jj}$ bins.","name":"Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t17","@type":"Dataset","description":"Distributions of $m_{T}^{WW}$ in the WW signal region.","name":"Figure 6a"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t18","@type":"Dataset","description":"Distributions of $m_{T}^{WZ}$ in the WZ signal region.","name":"Figure 6b"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t19","@type":"Dataset","description":"Observed and expected lower and upper 95\\% confidence level limits in TeV$^{-4}$ on the parameters of the quartic, obtained without...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.94181.v3/t20","@type":"Dataset","description":"Observed and expected lower and upper 95\\% confidence level limits in TeV$^{-4}$ on the parameters of the quartic by cutting...","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1794169?version=3"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/94181"}],"inLanguage":"en","name":"Measurements of production cross sections of WZ and same-sign WW boson pairs in association with two jets 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/ins1794169?version=3","version":3}