{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.113660.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1963239"}},{"@id":"https://doi.org/10.1007/JHEP03(2022)189","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2021","description":"The cross sections for inclusive and Mueller-Navelet dijet production are measured as a function of the rapidity separation between the jets in proton-proton collisions at $\\sqrt{s} =$ 2.76 TeV for jets with transverse momentum $p_\\mathrm{T}$$\\gt$ 35 GeV and rapidity $\\vert y\\vert$$\\lt$ 4.7. Various dijet production cross section ratios are also measured. A veto on additional jets with $p_\\mathrm{T}$$\\gt$ 20 GeV is introduced to improve the sensitivity to the effects of the Balitsky-Fadin-Kuraev-Lipatov (BFKL) evolution. The measurement is compared with the predictions of various Monte Carlo models based on leading-order and next-to-leading-order calculations including the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi leading-logarithm (LL) parton shower as well as the LL BFKL resummation.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t1","@type":"Dataset","description":"Summary of the systematic uncertainties on the cross section d\u03c3incl/d\u2206y.","name":"Figure 1-a"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t2","@type":"Dataset","description":"Summary of the systematic uncertainties on the cross section d\u03c3MN/d\u2206y.","name":"Figure 1-b"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t3","@type":"Dataset","description":"Summary of the systematic uncertainties on the ratio Rincl.","name":"Figure 1-c"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t4","@type":"Dataset","description":"Summary of the systematic uncertainties on the ratio RMN.","name":"Figure 1-d"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t5","@type":"Dataset","description":"Summary of the systematic uncertainties on the ratio Rincl_veto.","name":"Figure 1-e"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t6","@type":"Dataset","description":"Summary of the systematic uncertainties on the ratio RMN_veto.","name":"Figure 1-f"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t7","@type":"Dataset","description":"Differential cross section d\u03c3incl/d\u2206y for inclusive dijet production together with predictions of different MC models.","name":"Figure 2"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t8","@type":"Dataset","description":"Differential cross section d\u03c3MN/d\u2206y for Mueller-Navelet dijet production together with predictions of different MC models.","name":"Figure 3"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t9","@type":"Dataset","description":"Ratio Rincl of the cross sections for inclusive to \u201dexclusive\u201d dijet production together with predictions of different MC models.","name":"Figure 4"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t10","@type":"Dataset","description":"Ratio Rincl_veto of the cross sections for inclusive to \u201dexclusive\u201d with veto dijet production together with predictions of different MC...","name":"Figure 5"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t11","@type":"Dataset","description":"Ratio RMN of the cross sections for Mueller-Navelet to \u201dexclusive\u201d dijet production together with predicgtion of different MC models.","name":"Figure 6"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t12","@type":"Dataset","description":"Ratio RMN_veto of the cross sections for Mueller-Navelet to \u201dexclusive\u201d with veto dijet production together with predictions of different MC...","name":"Figure 7"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t13","@type":"Dataset","description":"Summary of the systematic uncertainties on the cross section d\u03c3incl/d\u2206y.","name":"Figure 5-a Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t14","@type":"Dataset","description":"Summary of the systematic uncertainties on the cross section d\u03c3MN/d\u2206y.","name":"Figure 5-b Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t15","@type":"Dataset","description":"Summary of the systematic uncertainties on the ratio Rincl.","name":"Figure 5-c Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t16","@type":"Dataset","description":"Summary of the systematic uncertainties on the ratio RMN.","name":"Figure 5-d Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t17","@type":"Dataset","description":"Summary of the systematic uncertainties on the ratio Rincl_veto.","name":"Figure 5-e Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t18","@type":"Dataset","description":"Summary of the systematic uncertainties on the ratio RMN_veto.","name":"Figure 5-f Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t19","@type":"Dataset","description":"Differential cross section d\u03c3incl/d\u2206y for inclusive dijet production together with predictions of different MC models.","name":"Figure 6 Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t20","@type":"Dataset","description":"Differential cross section d\u03c3MN/d\u2206y for Mueller-Navelet dijet production together with predictions of different MC models.","name":"Figure 7 Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t21","@type":"Dataset","description":"Ratio Rincl of the cross sections for inclusive to \u201dexclusive\u201d dijet production together with predictions of different MC models.","name":"Figure 8 Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t22","@type":"Dataset","description":"Ratio Rincl_veto of the cross sections for inclusive to \u201dexclusive\u201d with veto dijet production together with predictions of different MC...","name":"Figure 9 Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t23","@type":"Dataset","description":"Ratio RMN of the cross sections for Mueller-Navelet to \u201dexclusive\u201d dijet production together with predicgtion of different MC models.","name":"Figure 10 Supplementary"},{"@id":"https://doi.org/10.17182/hepdata.113660.v1/t24","@type":"Dataset","description":"Ratio RMN_veto of the cross sections for Mueller-Navelet to \u201dexclusive\u201d with veto dijet production together with predictions of different MC...","name":"Figure 11 Supplementary"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1963239?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/113660"}],"inLanguage":"en","name":"Study of dijet events with large rapidity separation in proton-proton collisions at $\\sqrt{s}$ = 2.76 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1963239?version=1","version":1}