![]() ![]() rĪlso at Borough of Manhattan Community College, City University of New York, New York City, United States of America. Petersburg State Polytechnical University, St. pĪlso at Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania. oĪlso at Institute of Particle Physics (IPP), Canada. nĪlso at Universita di Napoli Parthenope, Napoli, Italy. mĪlso at The Collaborative Innovation Center of Quantum Matter (CICQM), Beijing, China. lĪlso at Tomsk State University, Tomsk, and Moscow Institute of Physics and Technology State University, Dolgoprudny, Russia. kĪlso at Departamento de Fisica e Astronomia, Faculdade de Ciencias, Universidade do Porto, Portugal. jĪlso at Departament de Fisica de la Universitat Autonoma de Barcelona, Barcelona, Spain. iĪlso at II Physikalisches Institut, Georg-August-Universität, Göttingen, Germany. hĪlso at Department of Physics, University of Fribourg, Fribourg, Switzerland. gĪlso at Department of Physics, California State University, Fresno CA, United States of America. fĪlso at Physics Department, An-Najah National University, Nablus, Palestine. dĪlso at Department of Physics & Astronomy, University of Louisville, Louisville, KY, United States of America. cĪlso at Novosibirsk State University, Novosibirsk, Russia. bĪlso at Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan. Navigate Left Previous article in issueĪlso at Department of Physics, King's College London, London, United Kingdom.All search results are consistent with the expectations for the background due to Standard Model processes, and 95% CL upper limits are set, as a function of XH and X masses, on the production cross-section of the XH → q q ¯ ′ b b ¯ resonance. A two-dimensional phase space of XH mass versus X mass is scanned for evidence of a signal, over a range of XH resonance mass values between 1 TeV and 4 TeV, and for X particles with masses from 50 GeV to 1000 GeV. The search considers the regime of high XH resonance masses, where the X and H bosons are both highly Lorentz-boosted and are each reconstructed using a single jet with large radius parameter. The particle X is assumed to decay to a pair of light quarks, and the fully hadronic final state XH → q q ¯ ′ b b ¯ is analysed. A search for heavy resonances decaying into a Higgs boson ( H) and a new particle ( X) is reported, utilizing 36.1 fb −1 of proton–proton collision data at s = 13 TeV collected during 20 with the ATLAS detector at the CERN Large Hadron Collider. ![]()
0 Comments
Leave a Reply. |
AuthorWrite something about yourself. No need to be fancy, just an overview. ArchivesCategories |