{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.80169.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1629153"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-5691-6","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"Events with no charged particles produced between the two leading jets are studied in proton-proton collisions at $\\sqrt{s}$ = 7 TeV. The jets were required to have transverse momentum $p_\\mathrm{T}^{\\text{jet}}$ > 40 GeV and pseudorapidity 1.5 $<|\\eta^{\\text{jet}}| <$ 4.7, and to have values of $\\eta^{\\text{jet}}$ with opposite signs. The data used for this study were collected with the CMS detector during low-luminosity running at the LHC, and correspond to an integrated luminosity of 8 pb$^{-1}$. Events with no charged particles with $p_\\mathrm{T}$ > 0.2 GeV in the interval -1 < $\\eta$ < 1 between the jets are observed in excess of calculations that assume no color-singlet exchange. The fraction of events with such a rapidity gap, amounting to 0.5-1% of the selected dijet sample, is measured as a function of the $p_\\mathrm{T}$ of the second-leading jet and of the rapidity separation between the jets. The data are compared to previous measurements at the Tevatron, and to perturbative quantum chromodynamics calculations based on the Balitsky-Fadin-Kuraev-Lipatov evolution equations, including different modelings of the non-perturbative gap survival probability.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.80169.v1/t1","@type":"Dataset","description":"Measured values of Color Singlet Exchange fraction as a function of $p_{T}^{jet2}$","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.80169.v1/t2","@type":"Dataset","description":"Measured values of Color Singlet Exchange fraction as a function of mean $\\Delta\\eta_{jj}$ for $p_{T}^{jet2}$ 40-60 GeV","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.80169.v1/t3","@type":"Dataset","description":"Measured values of Color Singlet Exchange fraction as a function of mean $\\Delta\\eta_{jj}$ for $p_{T}^{jet2}$ 60-100 GeV","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.80169.v1/t4","@type":"Dataset","description":"Measured values of Color Singlet Exchange fraction as a function of mean $\\Delta\\eta_{jj}$ for $p_{T}^{jet2}$ 100-200 GeV","name":"Table 4"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1629153?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/80169"}],"inLanguage":"en","name":"Study of dijet events with a large rapidity gap between the two leading jets in pp collisions at $\\sqrt{s}$ = 7 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1629153?version=1","version":1}