Enriching the Standard Model & Beyond IAS Workshop Jan 27, 2012 Nanyang Technological University Singapore.

Slides:

Advertisements

Similar presentations

Towards a New Standard Model IUPAP Working Group 9 JULY 2, 2010 Stuart Freedman University of California at Berkeley and Lawrence Berkeley National Laboratory.

Advertisements

Resonant Leptogenesis In S4 Model Nguyen Thanh Phong Cantho University In cooperation with Prof. CSKim, SKKang and Dr. YHAhn (work in progress)

Outlook: Higgs, SUSY, flavor Ken-ichi Hikasa (Tohoku U.) Fourth Workshop, Origin of Mass and SUSY March 8, 2006, Epochal Tsukuba.

The minimal B-L model naturally realized at TeV scale Yuta Orikasa(SOKENDAI) Satoshi Iso(KEK,SOKENDAI) Nobuchika Okada(University of Alabama) Phys.Lett.B676(2009)81.

The classically conformal B-L extended standard model Yuta Orikasa Satoshi Iso(KEK,SOKENDAI) Nobuchika Okada(University of Alabama) Phys.Lett.B676(2009)81.

How to Evade a NO-GO Theorem in Flavor Symmetries Yoshio Koide (Osaka University) International Workshop on Grand Unified Theories: Current Status and.

Compelling Questions of High Energy Physics? What does the future hold? Persis S. Drell Physics Department Cornell University.

Higgs Boson Mass In Gauge-Mediated Supersymmetry Breaking Abdelhamid Albaid In collaboration with Prof. K. S. Babu Spring 2012 Physics Seminar Wichita.

Higgs Quadruplet for Type III Seesaw and Implications for → e and −e Conversion Ren Bo Coauther : Koji Tsumura, Xiao - Gang He arXiv:

Hadronic EDMs in SUSY GUTs

June 18, 2004Mitsuru Kakizaki1 Democratic (s)fermions and lepton flavor violation Mitsuru Kakizaki (ICRR, University of Tokyo) June 18, 2004 We propose.

Enriching the Standard Model With a family of CP even and odd Higgs fields IAS School Jan 13, 2012 Nanyang Technological University Singapore.

May 25, 2004Kakizaki, Mitsuru1 Flavor structure in supersymmetric models Kakizaki, Mitsuru (ICRR, University of Tokyo) May 25, 2004 We proposed a new alignment.

Aug. 16, 2003Mitsuru Kakizaki1 Democratic (s)fermions and lepton flavor violation Mitsuru Kakizaki （ Tohoku Univ. ） Aug. 16, 2003 Ref.: K. Hamaguchi, M.

Oct. 25, 2004Mitsuru Kakizaki1 Flavor structure in supersymmetric models Mitsuru Kakizaki (ICRR, University of Tokyo) Oct. 25, Ochanomizu University.

Enriching the Standard Model With a family of CP even and odd Higgs fields IAS School Jan 10, 2012 Nanyang Technological University Singapore.

B. Dutta Texas A&M University Phys.Rev.Lett.100:181801,2008; arXiv: ; To appear Grand Unified Models, Proton Decay and Phase of Collaborator: Yukihiro.

Probing Majorana Neutrinos in Rare Meson Decays Claudio Dib UTFSM I.S. & B.K. Fest, UTFSM, May 2010 G. Cvetic, C.D., S.K. Kang, C.S. Kim, PRD 82, ,

Neutrino Physics - Lecture 1 Steve Elliott LANL Staff Member UNM Adjunct Professor ,

Chiral freedom and the scale of weak interactions.

4 th Generation Leptons in Minimal Walking Technicolor Theory Matti Heikinheimo University of Jyväskylä.

July 19, 2005Mitsuru Kakizaki1 Hadronic EDMs in SUSY GUTs Mitsuru Kakizaki (ICRR, Univ. of Tokyo) July 19, IPPP We investigate hadronic EDMs induced.

Fermion Masses and Unification Steve King University of Southampton.

July 12, 2005Mitsuru Kakizaki1 Hadronic EDMs in SUSY GUTs Mitsuru Kakizaki (ICRR, Univ. of Tokyo) July 12, Nagoya University We investigate hadronic.

Aug 29-31, 2005M. Jezabek1 Generation of Quark and Lepton Masses in the Standard Model International WE Heraeus Summer School on Flavour Physics and CP.

Fermion Masses G.G.Ross, Corfu, September 2005 The Standard Model.

2-nd Vienna Central European Seminar, Nov 25-27, Rare Meson Decays in Theories Beyond the Standard Model A. Ali (DESY), A. V. Borisov, M. V. Sidorova.

What is mSUGRA? Physics in Progress, seminar talk, 11 th Feb 2010 Helmut Eberl.

Electroweak interaction

Minimal SO(10)×A4 SUSY GUT ABDELHAMID ALBAID In Collaboration with K. S. BABU Oklahoma State University.

The Standard Model of Electroweak Physics Christopher T. Hill Head of Theoretical Physics Fermilab.

2. Two Higgs Doublets Model

Probing Majorana Neutrinos (in Rare Decays of Mesons) 11/17/ DBD11 C. S. Kim arXiv: (PRD82,053010,2010) G. Cvetic, C. Dib, S.K. Kang, C.S.

Texture of Yukawa coupling matrices in general two-Higgs doublet model Yu-Feng Zhou J. Phys. G: Nucl. Part. Phys.30 (2004) Presented by Ardy.

Family Symmetry Solution to the SUSY Flavour and CP Problems Plan of talk: I.Family Symmetry II.Solving SUSY Flavour and CP Problems Work with and Michal.

Sally Dawson, BNL Introduction to the Standard Model TASI, 2006 Introduction to the Standard Model –Review of the SU(2) x U(1) Electroweak theory –Experimental.

QFD, Weak Interactions Some Weak Interaction basics

Neutrino mass and DM direct detection Daijiro Suematsu (Kanazawa Univ.) Erice Sept., 2013 Based on the collaboration with S.Kashiwase PRD86 (2012)

weak decays beta decay ofneutron problem energy and momentum not conserved e n p.

Duality in Left-Right Symmetric Seesaw Mechanism Michele Frigerio Service de Physique Théorique, CEA/Saclay Rencontres de Physique des Particules March.

Sally Dawson, BNL Standard Model and Higgs Physics FNAL LHC School, 2006 Introduction to the Standard Model  Review of the SU(2) x U(1) Electroweak theory.

Parity Symmetry at High- Energy: How High? Xiangdong Ji U of Maryland In collaboration with Zhang Yue An Haipeng R.N. Mohapatra.

DYNAMICAL GENERATION OF FERMION MASSES AND ITS CONSEQUENCES Jiří Hošek Department of Theoretical Physics Nuclear Physics Institute Rez (Prague) Czech Republic.

Charged Higgs boson at the LHC 이강영 ( 건국대학교 연세대학교

BEYOND MFV IN FAMILY SYMMETRY THEORIES OF FERMION MASSES Work done with Zygmunt Lalak and Graham Ross Based on existing ideas but, hopefully, contributing.

SUSY GUT Predictions for Neutrino Oscillation Mu-Chun Chen Brookhaven National Laboratory DUSEL Workshop, January 4-7, 2005 University of Colorado at Boulder.

Introduction to Flavor Physics in and beyond the Standard Model Enrico Lunghi References: The BaBar physics book,

Physics 222 UCSD/225b UCSB Lecture 12 Chapter 15: The Standard Model of EWK Interactions A large part of today’s lecture is review of what we have already.

Systematic model building... based on QLC assumptions NuFact 07 Okayama University, Japan August 8, 2007 Walter Winter Universität Würzburg.

Hunting for Hierarchies in PSL 2 (7) MICHAEL JAY PEREZ PHENOMENOLOGY 2015 MAY 5, 2015 ARXIV : /

1-2 Mass Degeneration in the Leptonic Sector Hiroyuki ISHIDA (Tohoku University) Collaboration with : Takeshi ARAKI (MISC) Ref ; T. Araki and H.I. arXiv.

2 Challenging Reveal physics beyond the Standard Model Unique opportunity to measure Standard Model parameters Precision test of the Standard Model “New.

and what we unsuccessfully tried to explain (so far)

Pontecorvo’s idea An introductory course on neutrino physics (IV)

A New Family Symmetry: Discrete Quaternion Group

Flavour Physics in and beyond the Standard Model

TeV-Scale Leptogenesis and the LHC

Reference: “The Standard Model Higgs Boson” by Ivo van Vulpen,

Hadronic EDMs in SUSY GUTs

The Flavour Problem and Family Symmetry

Flavor changing amplitudes in the littlest Higgs model with T-parity

Quark and lepton masses

Methods of Experimental Particle Physics

Yasuhiro Okada (KEK/Sokendai) October 18, 2007

Spontaneous breakdown (SB) of symmetry

Neutrino Oscillations

Lecture 12 Chapter 15: The Standard Model of EWK Interactions

Theoretical Status of LFV and Rare Tau decays

Higgs phenomena in economical models

A solution to the Strong CP problem with a softly broken CP symmetry

Presentation transcript:

Enriching the Standard Model & Beyond IAS Workshop Jan 27, 2012 Nanyang Technological University Singapore

The Standard Model

The Standard Model Lagrangian

The Yukawa Coupling lepton

Enriching the Standard Model

The New Higgs Field symmetric Anti- symmetric

The New Higgs Field Maximal CP violation

Fermion Mass Matrix Results by Gupta

Fermion Mass Matrix

Cabibbo Kobayashi-Maskawa Matrix Results by Gupta

Symmetric Lepton Mass Matrix

Transformation to Mass Eigenstates Lepton Mass Matrix

See-Saw Mechanism Flavor Neutrino Mass Matrix Lepton Mass Matrix

See-Saw Mechanism Flavor Neutrino Mass Marix Lepton Mass Matrix

and the is the diagonal mass matgrix for the heavy right-handed neutrinos

Type II Degeneracy

Type I Degeneracy

a =

PMNS Matrix

Experimental Indications Gulsheen Ahuja Type I Degeneracy a =

The Higgs Potential

Laplacian.wordpress.com

Spontaneous Symmetry Breaking New Vacuum

Spontaneous Symmetry Breaking Nambu-Goldstone Bosons

Fermion Mass Matrix Mass Hierarchy

The New Higgs Potential Tree Level Higgs Potential with minimum at new vacuum

The New Higgs Potential New Vacuum

The Higgs Potential Goldstone Bosons Up Quark Sector

The Higgs Potential Physical Higgs Field Up Quark Sector

The Higgs Potential PseudoGoldstone Bosons

The Higgs Potential PseudoGoldstone Bosons

Soft Breaking Terms Markos Maniatis

Flavor Diagonality

Penguin Diagrams

Flavor Diagonality Flavor Changing Amplitude

FCNC condition Flavor Diagonality

FCNC condition Flavor Diagonality

FCNC condition Flavor Diagonality

FCNC condition Flavor Diagonality

FCNC condition Flavor Diagonality

Enriching the Standard Model Implications for LHC 1.Higgs family has a rich hierarchy While some are heavy to conform to constraints from rare decays, there will be some `pseudo-Goldstone bosons’ that are low. 2.The Higgs bosons are not CP eigenstates and so there will be analogs of K L and K S oscillations. 3.The parameters of CKM matrices related to the hierarchies of Higgs family.

OPERA Underground Detector

Frontiers of Science Implications for Technology OPERA Experiment

& Beyond Superluminal neutrino? Chodos, Hauser & Kostelecky, 1985

& Beyond Superluminal neutrino?

& Beyond Equations of Motion

& Beyond

Structure of the In Vacuum

Structure of the Out Vacuum

Structure of the Vacua & Beyond

Micro-Causality & Beyond

Micro-Causality & Beyond

Neutrino Oscillation & Beyond

Neutrino Oscillation & Beyond

Neutrino Oscillation & Beyond

Neutrino Oscillation & Beyond

Tritium beta-decay

arXiv:hep-ph/ v1