{"title":"在$\\sqrt{s}$ = 13 TeV质子-质子对撞中测量德雷尔-扬前后不对称和有效轻子弱混合角","authors":"CMS Collaboration","doi":"arxiv-2408.07622","DOIUrl":null,"url":null,"abstract":"The forward-backward asymmetry in Drell-Yan production and the effective\nleptonic electroweak mixing angle are measured in proton-proton collisions at\n$\\sqrt{s}$ = 13 TeV, collected by the CMS experiment and corresponding to an\nintegrated luminosity of 138 fb$^{-1}$. The measurement uses both dimuon and\ndielectron events, and is performed as a function of the dilepton mass and\nrapidity. The unfolded angular coefficient $A_4$ is also extracted, as a\nfunction of the dilepton mass and rapidity. Using the CT18Z set of parton\ndistribution functions, we obtain $\\sin\\theta^\\ell_\\text{eff}$ = 0.23157 $\\pm$\n0.00031, where the uncertainty includes the experimental and theoretical\ncontributions. The measured value agrees with the standard model fit result to\nglobal experimental data. This is the most precise $\\sin\\theta^\\ell_\\text{eff}$\nmeasurement at a hadron collider, with a precision comparable to the results\nobtained at LEP and SLD.","PeriodicalId":501181,"journal":{"name":"arXiv - PHYS - High Energy Physics - Experiment","volume":"15 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Measurement of the Drell--Yan forward-backward asymmetry and of the effective leptonic weak mixing angle in proton-proton collisions at $\\\\sqrt{s}$ = 13 TeV\",\"authors\":\"CMS Collaboration\",\"doi\":\"arxiv-2408.07622\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The forward-backward asymmetry in Drell-Yan production and the effective\\nleptonic electroweak mixing angle are measured in proton-proton collisions at\\n$\\\\sqrt{s}$ = 13 TeV, collected by the CMS experiment and corresponding to an\\nintegrated luminosity of 138 fb$^{-1}$. The measurement uses both dimuon and\\ndielectron events, and is performed as a function of the dilepton mass and\\nrapidity. The unfolded angular coefficient $A_4$ is also extracted, as a\\nfunction of the dilepton mass and rapidity. Using the CT18Z set of parton\\ndistribution functions, we obtain $\\\\sin\\\\theta^\\\\ell_\\\\text{eff}$ = 0.23157 $\\\\pm$\\n0.00031, where the uncertainty includes the experimental and theoretical\\ncontributions. The measured value agrees with the standard model fit result to\\nglobal experimental data. This is the most precise $\\\\sin\\\\theta^\\\\ell_\\\\text{eff}$\\nmeasurement at a hadron collider, with a precision comparable to the results\\nobtained at LEP and SLD.\",\"PeriodicalId\":501181,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Physics - Experiment\",\"volume\":\"15 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-08-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Physics - Experiment\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2408.07622\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Experiment","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.07622","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Measurement of the Drell--Yan forward-backward asymmetry and of the effective leptonic weak mixing angle in proton-proton collisions at $\sqrt{s}$ = 13 TeV
The forward-backward asymmetry in Drell-Yan production and the effective
leptonic electroweak mixing angle are measured in proton-proton collisions at
$\sqrt{s}$ = 13 TeV, collected by the CMS experiment and corresponding to an
integrated luminosity of 138 fb$^{-1}$. The measurement uses both dimuon and
dielectron events, and is performed as a function of the dilepton mass and
rapidity. The unfolded angular coefficient $A_4$ is also extracted, as a
function of the dilepton mass and rapidity. Using the CT18Z set of parton
distribution functions, we obtain $\sin\theta^\ell_\text{eff}$ = 0.23157 $\pm$
0.00031, where the uncertainty includes the experimental and theoretical
contributions. The measured value agrees with the standard model fit result to
global experimental data. This is the most precise $\sin\theta^\ell_\text{eff}$
measurement at a hadron collider, with a precision comparable to the results
obtained at LEP and SLD.