PPT-- Global fit to precision electroweak data,

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. Chapter 1 Section 2. Accuracy. describes how close a measured value is to the true value of the quantity measured. . . a.k.a. “the right answer”, or the agreed upon answer (“consensus” among scientists). 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. Chapter 1 Section 2. Accuracy. describes how close a measured value is to the true value of the quantity measured. . . a.k.a. “the right answer”, or the agreed upon answer (“consensus” among scientists). Jeff Pool. March 19. th. , 2012. Motivation. Why energy?. It matters everywhere:. - Mobile devices. - Desktop computers. - Servers, data centers. It’s a bottleneck to performance!. 2. http://img717.imageshack.us/img717/3936/1101771coolitomni.jpg. DREAM . BIG. Dr. Shoumen Datta. The wealth of nations can’t depend only on. . castles in the cloud.. EMERGING. PLATFORM. ECONOMY. Peter Evans. 4. SMART CITIES . . . http. ://. bit.ly/GLOBAL-SIM-CITIES. CONTEXT. There are two . contexts precision . and accuracy apply to: sets of data, and measuring instruments.. In a set of data, those measures give an idea of the spread and “. ballpark. ” of the answer (final measurement).. Accuracy of a measurement:. An indication of how close the measurement is to the accepted value. Percentage difference can be calculated to give a quantitative indication of a measurement’s accuracy—the smaller the percentage difference, the greater the . 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. 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. 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:. 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.