CP Properties of Higgs Boson Interactions with Top Quarks in the t¯tH and tH Processes Using H → γγ with the ATLAS Detector
Metadatos
Afficher la notice complèteEditorial
American Physical Society
Date
2020-08-05Referencia bibliográfica
Aad, G., Abbott, B., Abbott, D. C., Abud, A. A., Abeling, K., Abhayasinghe, D. K., ... & Abreu, H. (2020). C P Properties of Higgs Boson Interactions with Top Quarks in the t t¯ H and t H Processes Using H→ γ γ with the ATLAS Detector. Physical review letters, 125(6), 061802. [DOI: 10.1103/PhysRevLett.125.061802]
Patrocinador
ANPCyT; YerPhI, Armenia; Australian Research Council; BMWFW, Austria; Austrian Science Fund (FWF); Azerbaijan National Academy of Sciences (ANAS); SSTC, Belarus; National Council for Scientific and Technological Development (CNPq); Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP); Natural Sciences and Engineering Research Council of Canada; NRC, Canada; Canada Foundation for Innovation; CERN; Comision Nacional de Investigacion Cientifica y Tecnologica (CONICYT); Chinese Academy of Sciences; Ministry of Science and Technology, China; National Natural Science Foundation of China (NSFC); Departamento Administrativo de Ciencia, Tecnologia e Innovacion Colciencias; Ministry of Education, Youth & Sports - Czech Republic Czech Republic Government; Czech Republic Government; DNRF, Denmark; Danish Natural Science Research Council; Centre National de la Recherche Scientifique (CNRS); CEA-DRF/IRFU, France; SRNSFG, Georgia; Federal Ministry of Education & Research (BMBF); HGF, Germany; Max Planck Society; Greek Ministry of Development-GSRT; RGC, China; Hong Kong SAR, China; Israel Science Foundation; Benoziyo Center, Israel; Istituto Nazionale di Fisica Nucleare (INFN); Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT) Japan Society for the Promotion of Science; CNRST, Morocco; Netherlands Organization for Scientific Research (NWO) Netherlands Government; RCN, Norway; Ministry of Science and Higher Education, Poland; NCN, Poland; Portuguese Foundation for Science and Technology; MNE/IFA, Romania; MES of Russia, Russia Federation; NRC KI, Russia Federation; JINR; MESTD, Serbia; MSSR, Slovakia; Slovenian Research Agency - Slovenia; MIZS, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC, Sweden; Wallenberg Foundation, Sweden; SERI, Switzerland; Swiss National Science Foundation (SNSF); Canton of Bern, Switzerland; Cantons of Geneva, Switzerland; Ministry of Science and Technology, Taiwan; Ministry of Energy & Natural Resources - Turkey; Science & Technology Facilities Council (STFC); United States Department of Energy (DOE); National Science Foundation (NSF); BCKDF, Canada; CANARIE, Canada; Compute Canada, Canada; CRC, Canada; European Union (EU) European Research Council (ERC); European Union (EU); Horizon 2020, European Union; European Union (EU); COST, European Union; French National Research Agency (ANR); German Research Foundation (DFG); Alexander von Humboldt Foundation; Herakleitos program - EU-ESF, Greece; Thales program - EU-ESF, Greece; Aristeia program - EU-ESF, Greece; Greek NSRF, Greece; BSF-NSF, Israel; German-Israeli Foundation for Scientific Research and Development; CERCA Programme Generalitat de Catalunya, Spain; PROMETEO Programme Generalitat Valenciana, Spain; Goran Gustafssons Stiftelse, Sweden; Royal Society of London; Leverhulme TrustRésumé
A study of the charge conjugation and parity (CP) properties of the interaction between the Higgs boson
and top quarks is presented. Higgs bosons are identified via the diphoton decay channel (H → γγ), and their
production in association with a top quark pair (t¯tH) or single top quark (tH) is studied. The analysis uses
139 fb−1 of proton–proton collision data recorded at a center-of-mass energy of ffiffi
s p ¼ 13 TeV with the
ATLAS detector at the Large Hadron Collider. Assuming a CP-even coupling, the t¯tH process is observed
with a significance of 5.2 standard deviations. The measured cross section times H → γγ branching ratio is
1.64þ0.38 −0.36 ðstatÞ
þ0.17 −0.14 ðsysÞ fb, and the measured rate for t¯tH is 1.43þ0.33 −0.31 ðstatÞ
þ0.21 −0.15 ðsysÞ times the Standard
Model expectation. The tH production process is not observed and an upper limit on its rate of 12 times the
Standard Model expectation is set. A CP-mixing angle greater (less) than 43 ð−43Þ° is excluded at
95% confidence level.