PPT-Texture of Yukawa coupling matrices in general two-Higgs doublet model

Author : stefany-barnette | Published Date : 2018-11-12

Yu Feng Zhou J Phys G Nucl Part Phys30 2004 783792 Presented by Ardy Introduction Unresolved problems within the SM the origin of the fermion masses mixing angles

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Texture of Yukawa coupling matrices in general two-Higgs doublet model: Transcript

Yu Feng Zhou J Phys G Nucl Part Phys30 2004 783792 Presented by Ardy Introduction Unresolved problems within the SM the origin of the fermion masses mixing angles and CP violation etc. Tim Wiser. Splash P2506. 3 Nov 2012. Plan . Standard Model of Particle Physics. Particles, interactions, and the Higgs field. Drawing Feynman diagrams. These simple pictures are actually . calculational. Review of Splitting. Caused by shift due to magnetic fields of adjacent protons. We say that these protons are “coupled”. Protons may be coupled to different degrees. Coupling constant. Typically 7 Hz for adjacent sp. . with Type-II. Nambu. -Goldstone Boson. . Based on arXiv:1102.4145v2 [. hep. -ph]. Yusuke Hama. 　. (Univ. Tokyo). Tetsuo . Hatsuda. (Univ. Tokyo). Shun Uchino (Kyoto Univ.). 4/20 (2011). 　. Dense Strange Nuclei and Compressed Baryonic Matter. . Aungshuman. . Zaman. Department of Physics and Astronomy. Stony Brook University. October 11, 2010. What Is This Talk All About. Why is the search for the Higgs Boson important?. Gauge theory and standard model.. : data . vs. theory. Joey Huston. Bruce . Mellado. 1. Higgs(->. gg. )+jets. Most of the excess observed for Higgs production is in >=1 jet final states. Maybe CMS does not see as large of an excess. M. Veltman. NIKHEF. Amsterdam. Cern, 4 dec. 2009. Higgs search. Higgs hunting. In 1974 I asked myself: if the Higgs is all around us in the vacuum. we should really be able to see it. Since the Higgs field in the vacuum. Injection of long bunches into . SPS, capture of . each bunch in 2 neighboring 200 MHz buckets. Successfully tested in MDs . at . 2. 012. /13 run with . 1.65x10. 11. . p/doublet . Clear enhancement on . Hananeh. . Saghiha. Standard model. 12 fermions. Quarks & leptons. Some carry color charge. Some carry electric charge. Classified to 3 generations. Gauge bosons as force . carriers. Figures from . Christian Grefe, . Tomáš Laštovička. , Blai Pie Valls, Jan Strube and Frederic Teubert . WG6 Meeting . 16/02/2011. Channels Summary. H→. μμ. Very rare decay (≈5.10. -4. ). Difficult to observe at the LHC (3. Revolutionizing the Laws of the Universe with the LHC. Ashutosh Kotwal. Duke University. Egyptian Pyramids: Monument for Glory. Great Wall of China: Monument for Defense. Monument for Knowledge: The Large . In particle physics , elementary particles and forces give rise to the world around us.. The two main elementary particles which form the major constituent of matter are the LEPTONS and QUARKS.. Quark+Quark=hadrons [protons&neutrons].. M. Veltman. NIKHEF. Amsterdam. Cern, 4 dec. 2009. Higgs search. Higgs hunting. In 1974 I asked myself: if the Higgs is all around us in the vacuum. we should really be able to see it. Since the Higgs field in the vacuum. and LHC. :. la . grande. . sfida. . della. . Nuova. . Fisica. Antonio Masiero. Univ. di Padova e INFN. Univ. di Napoli, . Dipt. . Di . Fisica. , 15 . giugno. 2012. FCNC, CP ≠, (g-2), (. ). Rotation of coordinates -the rotation matrixStokes Parameters and unpolarizedlight1916 -20041819 -1903Hans Mueller1900 -1965yyxyEEEElinear arbitrary anglepolarization right or left circularpolarizati

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