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. 1. H. (Proton) NMR . Spectra. 1. number of signals. 2. their intensity (as measured by area . under peak). 3. splitting pattern (multiplicity). Information contained in an NMR. spectrum includes:. Yuta. . Orikasa. (SOKENDAI). Satoshi . Iso. (KEK,SOKENDAI). Nobuchika. Okada(University of Alabama). Phys.Lett.B676(2009)81. Phys.Rev.D80(2009)115007. The Standard Model is the best theory of describing the nature of particle physics, which is in excellent agreement with almost of all current experiments.. 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. Higgs . Dark . M. atter . & . Its Collider . Signals. ・ . E. . Asakawa, M. Asano, K. Fujii, T. Kusano, S. . M., R. . Sasaki. ,. Y. . Takubo, and H. . Yamamoto, PRD 79, 2009.. ・ . S. . . M, . 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. . mirrors. . for. a light . Higgs. Iván . Davidovich. Instituto . Balseiro. . & CONICET. In . collaboration. . with. E. Andrés and L. Da . Rold. Fermilab. , 10/20/15. ATLAS + CMS . But . radiative. S. Dawson. CMS HH Workshop. January 18, 2016. 1. S. Dawson. Outline. Why measure the Higgs-self couplings?. What do we expect?. Standard Model. Issues with the top mass dependence. Beyond the Standard Model. Kei . Yagyu. . (National Central U). M. Aoki, S. . Kanemura. , KY, PRD85 (2012), . S. . Kanemura. , KY, PRD85 (2012), . M. Aoki, S. . Kanemura. , M. Kikuchi, KY, PLB714 (2012), . M. Aoki, S. . Kanemura. (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. (General Overview). 1. Shaaban Khalil. Center . for . Fundamental Physics . Zewail. City of Science and Technology. The Standard Model. Standard . Model . is defined by. 4-dimension . QFT (Invariant under Poincare group. 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. Kathryn Grimm. Lancaster University. on behalf of the ATLAS and CMS . collaborations. HEFT 2017, Lumley Castle. Kathryn Grimm. Outline. The newest and best measurements for Higgs couplings, cross sections, and . Ranjan. . Modak. &. Debabrata. . Pramanik. Outline of talk... SU(5). Sub-algebra of SU(5). Branching Rule for diff rep of SU(5). Unification and why SU(5)?. Proton decay. SU(5). Cartan. generators for SU(5): 4 rank algebra its has 4 simple roots and 4 . ACFI EDM School November 2016. M.J. Ramsey-Musolf. U Mass Amherst. http://www.physics.umass.edu/acfi/. 2. Lecture IV Outline. General Considerations. BSM Motivation. Supersymmetry (Minimal Model). Higgs Portal CPV: 2 Higgs Doublet Model.

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