{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.103064.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1846679"}},{"@id":"https://doi.org/10.1103/PhysRevD.104.032006","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2021","description":"Many new physics models, including versions of supersymmetry characterized by $R$-parity violation (RPV), compressed mass spectra, long decay chains, or additional hidden sectors, predict the production of events with top quarks, low missing transverse momentum, and many additional quarks or gluons. The results of a search for new physics in events with two top quarks and additional jets are reported. The search is performed using events with at least seven jets and exactly one electron or muon. No requirement on missing transverse momentum is imposed. The study is based on a sample of proton-proton collisions at $\\sqrt{s} =$ 13 TeV corresponding to 137 fb$^{-1}$ of integrated luminosity collected with the CMS detector at the LHC in 2016-2018. The data are used to determine best fit values and upper limits on the cross section for pair production of top squarks in scenarios of RPV and stealth supersymmetry. Top squark masses up to 670 (870) GeV are excluded at 95% confidence level for the RPV (stealth) scenario, and the maximum observed local signal significance is 2.8 standard deviations for the RPV scenario with top squark mass of 400 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t1","@type":"Dataset","description":"Fitted background prediction and observed data counts for 2016 as functions of $N_{\\text{jets}}$ in each of the four $S_{\\textrm{NN}}$ bins....","name":"Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t2","@type":"Dataset","description":"Fitted background prediction and observed data counts for 2017 as functions of $N_{\\text{jets}}$ in each of the four $S_{\\textrm{NN}}$ bins....","name":"Figure 4b"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t3","@type":"Dataset","description":"Fitted background prediction and observed data counts for 2018A as functions of $N_{\\text{jets}}$ in each of the four $S_{\\textrm{NN}}$ bins....","name":"Figure 4c"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t4","@type":"Dataset","description":"Fitted background prediction and observed data counts for 2018B as functions of $N_{\\text{jets}}$ in each of the four $S_{\\textrm{NN}}$ bins....","name":"Figure 4d"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t5","@type":"Dataset","description":"Expected and observed 95% CL upper limit on the top squark pair production cross section as a function of the...","name":"Figure 6a"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t6","@type":"Dataset","description":"Expected and observed 95% CL upper limit on the top squark pair production cross section as a function of the...","name":"Figure 6b"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t7","@type":"Dataset","description":"Cut flow of the signal region selection decribed in section II.","name":"Signal cutflow 2016"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t8","@type":"Dataset","description":"Cut flow of the signal region selection decribed in section II.","name":"Signal cutflow 2017"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t9","@type":"Dataset","description":"Cut flow of the signal region selection decribed in section II.","name":"Signal cutflow 2018A"},{"@id":"https://doi.org/10.17182/hepdata.103064.v1/t10","@type":"Dataset","description":"Cut flow of the signal region selection decribed in section II.","name":"Signal cutflow 2018B"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1846679?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/103064"}],"inLanguage":"en","name":"Search for top squarks in final states with two top quarks and several light-flavor 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/ins1846679?version=1","version":1}