PPT-Global fit to dimension-6 operators using precision electroweak data, W+W- at LEP, Higgs

diboson data from LHC Runs 1 and 2 Results in Warsaw and SILH bases Improvements in the constraints from Run 2 Constraints on BSM models Some contribute to operators at tree level Stops that contribute at loop level. of . the Standard . Model after . the discovery of an SM-like scalar boson. Andreas Hoecker (CERN). Solvay . workshop . “. Facing . the Scalar . Sector. ”, . May . 29. -. 31, . 2013 . Introduction. (possible) . Higgs Boson at the LHC . Amitabh Lath. Rutgers, The State University of New Jersey. August 7, 2012. Statement by CERN DG on 7/4. Statement by CERN DG on 7/4. What’ he talking about?. Isn. after the Higgs Discovery. M.V. . Chizhov. Sofia University, Bulgaria and JINR, Russia. 09/06/2014. 2. Why do we need the Higgs boson?. S = ½. S = 1. S = 0. 09/06/2014. Harmonic Oscillator. (Analytical . Fermilab. , 14-16 . Nov.2012. The . Higgs Boson Discovery. 4. th. July . 2012. Discovered Higgs-like Boson. : Clear mass peak in . gg. and ZZ*. 4. l. I. s this the SM one ? From searches to measurements. Herwig. . Schopper’s. 90. th. birthday. John Ellis. (King’s College London & CERN). LEP1: the Ascent of the Standard Model. The Historical Context - I. 1964 – The . Englert. -. Brout. -Higgs mechanism. Pb+Pb. and . p. +Pb. collision from the ATLAS Detector at the LHC.. Alexander Milov. For the ATLAS Collaboration. Sasha Milov Electroweak probes with ATLAS IS2014 Napa, CA Dec. 5, 2014. Pb+Pb. and . p. +Pb. collision from the ATLAS Detector at the LHC.. Alexander Milov. For the ATLAS Collaboration. Sasha Milov Electroweak probes with ATLAS IS2014 Napa, CA Dec. 5, 2014. Higgs:. CP, . κ. V,f. , . flavour. violation, …. Electroweak:. sin. 2. θ, TGCs, …. Beyond SM:. Supersymmetry. ?. Composite models? . …. Standard Model EFT. Flavour. :. Top, . CKM, . …. New Accelerators:. LHC. FCC-. ee. FCC-. hh. HL-LHC Plans. Prospects . for HL-. LHC Higgs Measurements. Factors multiplying SM c. ouplings. Trilinear. Higgs c. oupling. Projected . e. +. e. -. Colliders:. Luminosity . The . Frontiers. of PP; . what. to do . next. ?. Strategy. Next. Accelerator . Technology. . C. hallenges . for . PP. Conclusion. Roy Aleksan. Nobel Symposium. May 13-17, 2013. m. H. . ~ . 125.5. FCCs. a story of . synergy. and . complementarity. . Photo . J. . Wenninger. Alain . Blondel, . University. of . Geneva. with. . many. . thanks. to the FCC . collaborators. !. . see. 1. Spontaneous symmetry breaking. in gauge theories. Tom Kibble. 20 Jan 2014. Electroweak symmetry breaking Jan 2014. 2. Symmetry. This talk is the story of how this idea . of spontaneous symmetry breaking . Tatsu Takeuchi. Virginia Tech. January 10, 2012. @ Osaka U. Part 1. 温故知新. （論語）. By scrutinizing existing Knowledge, . you can obtain New Knowledge. Example in Astronomy:. Discovery of Neptune:. W. +. W. −. at LEP,. Higgs . and . diboson. data from . LHC Runs . 1 and . 2. - Results in Warsaw . and SILH operator . bases. improvements . in the constraints . from LHC . Run . 2. - Constraints on BSM models.