{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.88816.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1737508"}},{"@id":"https://doi.org/10.1007/JHEP08(2019)150","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"A search for supersymmetric particles produced in the vector boson fusion topology in proton-proton collisions is presented. The search targets final states with one or zero leptons, large missing transverse momentum, and two jets with a large separation in rapidity. The data sample corresponds to an integrated luminosity of 35.9 fb$^{-1}$ of proton-proton collisions at $\\sqrt{s}=13$ TeV collected in 2016 with the CMS detector at the LHC. The observed dijet invariant mass and lepton-neutrino transverse mass spectra are found to be consistent with the standard model predictions. Upper limits are set on the cross sections for chargino ($\\tilde{\\chi}_{1}^{\\pm}$) and neutralino ($\\tilde{\\chi}_{2}^{0}$) production with two associated jets. For a compressed mass spectrum scenario in which the $\\tilde{\\chi}_{1}^{\\pm}$ and $\\tilde{\\chi}_{2}^{0}$ decays proceed via a light slepton and the mass difference between the lightest neutralino $\\tilde{\\chi}_{1}^{0}$ and the mass-degenerate particles $\\tilde{\\chi}_{1}^{\\pm}$ and $\\tilde{\\chi}_{2}^{0}$ is 1 (30) GeV, the most stringent lower limit to date of 112 (215) GeV is set on the mass of these latter two particles.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t1","@type":"Dataset","description":"Selection efficiency on signal for each channel.","name":"Signal efficiency"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t2","@type":"Dataset","description":"The observed $m_{T}$ and $m_{jj}$ distributions in the ejj (upper left), $\\mu$~jj (upper right), $\\tau_{h}$~jj (lower left), and $0\\ell$~jj (lower...","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t3","@type":"Dataset","description":"The observed $m_{T}$ and $m_{jj}$ distributions in the ejj (upper left), $\\mu$~jj (upper right), $\\tau_{h}$~jj (lower left), and $0\\ell$~jj (lower...","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t4","@type":"Dataset","description":"The observed $m_{T}$ and $m_{jj}$ distributions in the ejj (upper left), $\\mu$~jj (upper right), $\\tau_{h}$~jj (lower left), and $0\\ell$~jj (lower...","name":"Figure 3c"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t5","@type":"Dataset","description":"The observed $m_{T}$ and $m_{jj}$ distributions in the ejj (upper left), $\\mu$~jj (upper right), $\\tau_{h}$~jj (lower left), and $0\\ell$~jj (lower...","name":"Figure 3d"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t6","@type":"Dataset","description":"Combined 95% CL UL on the cross section as a function of $m(\\tilde{\\chi}_{2}^{0})=m(\\tilde{\\chi}_{1}^{\\pm})$. The results correspond to $\\Delta m=1$ GeV...","name":"Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t7","@type":"Dataset","description":"Combined 95% CL UL on the cross section as a function of $m(\\tilde{\\chi}_{2}^{0})=m(\\tilde{\\chi}_{1}^{\\pm})$. The results correspond to $\\Delta m=1$ GeV...","name":"Figure 4b"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t8","@type":"Dataset","description":"Combined 95% CL UL on the cross section as a function of $m(\\tilde{\\chi}_{2}^{0})=m(\\tilde{\\chi}_{1}^{\\pm})$. The results correspond to $\\Delta m=1$ GeV...","name":"Figure 4c"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t9","@type":"Dataset","description":"Combined 95% CL UL on the cross section as a function of $m(\\tilde{\\chi}_{2}^{0})=m(\\tilde{\\chi}_{1}^{\\pm})$. The results correspond to $\\Delta m=1$ GeV...","name":"Figure 4d"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t10","@type":"Dataset","description":"(Left) Expected and observed 95% confidence level upper limit (UL) on the signal cross section as a function of $m(\\tilde{\\chi}_{1}^{\\pm})$...","name":"Figure 5a 2D"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t11","@type":"Dataset","description":"(Left) Expected and observed 95% confidence level upper limit (UL) on the signal cross section as a function of $m(\\tilde{\\chi}_{1}^{\\pm})$...","name":"Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t12","@type":"Dataset","description":"(Left) Expected and observed 95% confidence level upper limit (UL) on the signal cross section as a function of $m(\\tilde{\\chi}_{1}^{\\pm})$...","name":"Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t13","@type":"Dataset","description":"(Left) Expected and observed 95% confidence level upper limit (UL) on the signal cross section as a function of $m(\\tilde{\\chi}_{1}^{\\pm})$...","name":"Figure 6a 2D"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t14","@type":"Dataset","description":"(Left) Expected and observed 95% confidence level upper limit (UL) on the signal cross section as a function of $m(\\tilde{\\chi}_{1}^{\\pm})$...","name":"Figure 6a"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t15","@type":"Dataset","description":"Example description","name":"Figure 6b"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t16","@type":"Dataset","description":"Combined 95% CL expected upper limit on the signal cross section as a function of $m_{\\tilde{\\chi}_{2}^{0}}=m_{\\tilde{\\chi}_{1}^{\\pm}}$ for a $\\Delta m=1$...","name":"Figure 7"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t17","@type":"Dataset","description":"Combined 95% CL expected upper limit on the signal cross section as a function of $m_{\\tilde{\\chi}_{2}^{0}}=m_{\\tilde{\\chi}_{1}^{\\pm}}$ for a $\\Delta m=50$...","name":"Figure 8"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t18","@type":"Dataset","description":"Combined 95% CL observed upper limit on the signal cross section as a function of $m_{\\tilde{\\chi}_{2}^{0}}=m_{\\tilde{\\chi}_{1}^{\\pm}}$ for a $\\Delta m=1$...","name":"Figure 9"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t19","@type":"Dataset","description":"Combined 95% CL observed upper limit on the signal cross section as a function of $m_{\\tilde{\\chi}_{2}^{0}}=m_{\\tilde{\\chi}_{1}^{\\pm}}$ for a $\\Delta m=50$...","name":"Figure 10"},{"@id":"https://doi.org/10.17182/hepdata.88816.v1/t20","@type":"Dataset","description":"Covariance matrix from the combined fit of the $m_{ extrm{jj}}$ and $m_{ extrm{T}}$ distributions in the $0\\ell extrm{jj}$ and $1\\ell...","name":"Figure 11"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1737508?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/88816"}],"inLanguage":"en","name":"Search for supersymmetry with a compressed mass spectrum in the vector boson fusion topology with 1-lepton and 0-lepton final states 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/ins1737508?version=1","version":1}