{"title":"利用质子-质子对撞在 $\\sqrt{s}$ = 13 TeV 发生的轻子+射流事件测量极化和自旋相关性并观测顶夸克对中的纠缠现象","authors":"CMS Collaboration","doi":"arxiv-2409.11067","DOIUrl":null,"url":null,"abstract":"Measurements of the polarization and spin correlation in top quark pairs\n($\\mathrm{t\\bar{t}}$) are presented using events with a single electron or muon\nand jets in the final state. The measurements are based on proton-proton\ncollision data from the LHC at $\\sqrt{s}$ = 13 TeV collected by the CMS\nexperiment, corresponding to an integrated luminosity of 138 fb$^{-1}$. All\ncoefficients of the polarization vectors and the spin correlation matrix are\nextracted simultaneously by performing a binned likelihood fit to the data. The\nmeasurement is performed inclusively and in bins of additional observables,\nsuch as the mass of the $\\mathrm{t\\bar{t}}$ system and the top quark scattering\nangle in the $\\mathrm{t\\bar{t}}$ rest frame. The measured polarization and spin\ncorrelation are in agreement with the standard model. From the measured spin\ncorrelation, conclusions on the $\\mathrm{t\\bar{t}}$ spin entanglement are drawn\nby applying the Peres-Horodecki criterion. The standard model predicts\nentangled spins for $\\mathrm{t\\bar{t}}$ states at the production threshold and\nat high masses of the $\\mathrm{t\\bar{t}}$ system. Entanglement is observed for\nthe first time in events at high $\\mathrm{t\\bar{t}}$ mass, where a large\nfraction of the $\\mathrm{t\\bar{t}}$ decays are space-like separated, with an\nexpected and observed significance of above 5 standard deviations.","PeriodicalId":501181,"journal":{"name":"arXiv - PHYS - High Energy Physics - Experiment","volume":"201 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Measurements of polarization and spin correlation and observation of entanglement in top quark pairs using lepton+jets events from proton-proton collisions at $\\\\sqrt{s}$ = 13 TeV\",\"authors\":\"CMS Collaboration\",\"doi\":\"arxiv-2409.11067\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Measurements of the polarization and spin correlation in top quark pairs\\n($\\\\mathrm{t\\\\bar{t}}$) are presented using events with a single electron or muon\\nand jets in the final state. The measurements are based on proton-proton\\ncollision data from the LHC at $\\\\sqrt{s}$ = 13 TeV collected by the CMS\\nexperiment, corresponding to an integrated luminosity of 138 fb$^{-1}$. All\\ncoefficients of the polarization vectors and the spin correlation matrix are\\nextracted simultaneously by performing a binned likelihood fit to the data. The\\nmeasurement is performed inclusively and in bins of additional observables,\\nsuch as the mass of the $\\\\mathrm{t\\\\bar{t}}$ system and the top quark scattering\\nangle in the $\\\\mathrm{t\\\\bar{t}}$ rest frame. The measured polarization and spin\\ncorrelation are in agreement with the standard model. From the measured spin\\ncorrelation, conclusions on the $\\\\mathrm{t\\\\bar{t}}$ spin entanglement are drawn\\nby applying the Peres-Horodecki criterion. The standard model predicts\\nentangled spins for $\\\\mathrm{t\\\\bar{t}}$ states at the production threshold and\\nat high masses of the $\\\\mathrm{t\\\\bar{t}}$ system. Entanglement is observed for\\nthe first time in events at high $\\\\mathrm{t\\\\bar{t}}$ mass, where a large\\nfraction of the $\\\\mathrm{t\\\\bar{t}}$ decays are space-like separated, with an\\nexpected and observed significance of above 5 standard deviations.\",\"PeriodicalId\":501181,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Physics - Experiment\",\"volume\":\"201 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-17\",\"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-2409.11067\",\"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-2409.11067","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Measurements of polarization and spin correlation and observation of entanglement in top quark pairs using lepton+jets events from proton-proton collisions at $\sqrt{s}$ = 13 TeV
Measurements of the polarization and spin correlation in top quark pairs
($\mathrm{t\bar{t}}$) are presented using events with a single electron or muon
and jets in the final state. The measurements are based on proton-proton
collision data from the LHC at $\sqrt{s}$ = 13 TeV collected by the CMS
experiment, corresponding to an integrated luminosity of 138 fb$^{-1}$. All
coefficients of the polarization vectors and the spin correlation matrix are
extracted simultaneously by performing a binned likelihood fit to the data. The
measurement is performed inclusively and in bins of additional observables,
such as the mass of the $\mathrm{t\bar{t}}$ system and the top quark scattering
angle in the $\mathrm{t\bar{t}}$ rest frame. The measured polarization and spin
correlation are in agreement with the standard model. From the measured spin
correlation, conclusions on the $\mathrm{t\bar{t}}$ spin entanglement are drawn
by applying the Peres-Horodecki criterion. The standard model predicts
entangled spins for $\mathrm{t\bar{t}}$ states at the production threshold and
at high masses of the $\mathrm{t\bar{t}}$ system. Entanglement is observed for
the first time in events at high $\mathrm{t\bar{t}}$ mass, where a large
fraction of the $\mathrm{t\bar{t}}$ decays are space-like separated, with an
expected and observed significance of above 5 standard deviations.