Book contents
- Frontmatter
- Dedication
- Contents
- Preface
- Acknowledgements
- List of Abbreviations
- Introduction
- Part I Basics of Gauge Theories
- Part II The StandardModel
- Part III Weak Decays in the StandardModel
- Part IV Weak Decays beyond the StandardModel
- 13 First Steps beyond the Standard Model
- 14 Standard Model Effective Field Theory
- 15 Simplest Extensions of the SM
- 16 Specific Models
- 17 Beyond Quark Flavor Physics
- 18 Grand Summary of New Physics Models
- 19 Flavor Expedition to the Zeptouniverse
- 20 Summary and Shopping List
- Appendix A Dirac Algebra, Spinors, Pauli and Gell-Mann Matrices
- Appendix B Feynman Rules of the Standard Model
- Appendix C Massive Loop Integrals
- Appendix D Numerical Input
- Appendix E Analytic Solutions to SMEFT RG Equations
- References
- Index
15 - Simplest Extensions of the SM
from Part IV - Weak Decays beyond the StandardModel
Published online by Cambridge University Press: 11 June 2020
- Frontmatter
- Dedication
- Contents
- Preface
- Acknowledgements
- List of Abbreviations
- Introduction
- Part I Basics of Gauge Theories
- Part II The StandardModel
- Part III Weak Decays in the StandardModel
- Part IV Weak Decays beyond the StandardModel
- 13 First Steps beyond the Standard Model
- 14 Standard Model Effective Field Theory
- 15 Simplest Extensions of the SM
- 16 Specific Models
- 17 Beyond Quark Flavor Physics
- 18 Grand Summary of New Physics Models
- 19 Flavor Expedition to the Zeptouniverse
- 20 Summary and Shopping List
- Appendix A Dirac Algebra, Spinors, Pauli and Gell-Mann Matrices
- Appendix B Feynman Rules of the Standard Model
- Appendix C Massive Loop Integrals
- Appendix D Numerical Input
- Appendix E Analytic Solutions to SMEFT RG Equations
- References
- Index
Summary
In order to illustrate what happens in specific models we will discuss three classes of models: the so-called 331 models, models with heavy vector-like quarks and models with leptoquarks, either of spin-0 or spin-1. We will concentrate on models with leptoquarks having sufficiently low masses so that they could be in principle discovered by the LHC. But even if the masses of new particles in the models considered will turn out to be beyond the reach of the LHC, their presence can still be identifiedin the rare processes discussed by us. These three classes of models are sufficiently simple so that we can present them here in some details. The new aspect of these models will be larger involvement of leptons than in previous sections. Yet, in thischapter we will confine the phenomenology to quark flavour observables postponing the discussion of lepton flavor violation to the next chapter. There are several more complicated models that we will only briefly mention providing list of references to papers investigatingweak decays in these models.
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- Gauge Theory of Weak Decays , pp. 466 - 532Publisher: Cambridge University PressPrint publication year: 2020