{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89049.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1711231"}},{"@id":"https://doi.org/10.1007/JHEP04(2019)114","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"A search for nonresonant excesses in the invariant mass spectra of electron and muon pairs is presented. The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment in 2016, corresponding to a total integrated luminosity of $36\\,\\text{fb}^{-1}$. No significant deviation from the standard model is observed. Limits are set at 95% confidence level on energy scales for two general classes of nonresonant models. For a class of fermion contact interaction models, lower limits ranging from 20 to 32 TeV are set on the characteristic compositeness scale $\\Lambda$. For the Arkani-Hamed, Dimopoulos, and Dvali model of large extra dimensions, the first results in the dilepton final state at 13 TeV are reported, and values of the ultraviolet cutoff parameter $\\Lambda_{\\text{T}}$ below 6.9 TeV are excluded. A combination with recent CMS diphoton results improves this exclusion to $\\Lambda_{\\text{T}}$ below 7.7 TeV, providing the most sensitive limits to date in nonhadronic final states.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t1","@type":"Dataset","description":"Electron pair invariant mass spectra for the combined barrel-barrel and barrel-endcap event categories. Example model predictions are given for CI....","name":"Dielectron mass distribution"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t2","@type":"Dataset","description":"Muon pair invariant mass spectra for the combined barrel-barrel and barrel-endcap event categories. Example model predictions are given for the...","name":"Dimuon mass distribution"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t3","@type":"Dataset","description":"Dilepton exclusion limits at 95% CL on the CI scale (Lambda) for the six CI models considered for the electron...","name":"Limits on the CI scale Lambda in the electron channel"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t4","@type":"Dataset","description":"Dilepton exclusion limits at 95% CL on the CI scale (Lambda) for the six CI models considered for the muon...","name":"Limits on the CI scale Lambda in the muon channel"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t5","@type":"Dataset","description":"Combined dilepton 95% CL exclusion limits on the cross section for the left-left constructive CI model. The red curve in...","name":"Combined limit on CI vs Lambda for the ConLL case"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t6","@type":"Dataset","description":"Combined dilepton 95% CL exclusion limits on the CI scale (Lambda) for the six different CI models considered. Thelimits are...","name":"Combined limits on the CI scale Lambda"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t7","@type":"Dataset","description":"Exclusion limits at 95% CL on the UV cutoff for the electron channel with m&gt; 1.8 TeV in the GRW,...","name":"Limits on the UV cutoff in the ADD model in the electron channel"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t8","@type":"Dataset","description":"Exclusion limits at 95% CL on the UV cutoff for the muon channel with m&gt; 1.8 TeV in the GRW,...","name":"Limits on the UV cutoff in the ADD model in the muon channel"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t9","@type":"Dataset","description":"Combined dilepton 95% CL exclusion limit on the cross section in the GRW convention with m &gt; 1.8 TeV for...","name":"Combined limit in the ADD model  vs the UV cutoff LambdaT"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t10","@type":"Dataset","description":"Combined dilepton 95% CL exclusion limits on the UV cutoff with m&gt; 1.8 TeV in the GRW, Hewett, and HLZ...","name":"Limits on the UV cutoff in the ADD model in the combined channel"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t11","@type":"Dataset","description":"Individual and combined dilepton (this analysis) and diphoton 95% CL expected exclusion limits as a summary of all parameter conventions...","name":"ADD expected limits combination of all channels"},{"@id":"https://doi.org/10.17182/hepdata.89049.v1/t12","@type":"Dataset","description":"Individual and combined dilepton (this analysis) and diphoton 95% CL observed exclusion limits as a summary of all parameter conventions...","name":"ADD observed limits combination of all channels"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1711231?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/89049"}],"inLanguage":"en","name":"Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at $\\sqrt{s}=$ 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1711231?version=1","version":1}
