Grand Unified Theories and Supersymmetry in Particle Physics
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Report of the Supersymmetry Theory Subgroup
Report of the Supersymmetry Theory Subgroup J. Amundson (Wisconsin), G. Anderson (FNAL), H. Baer (FSU), J. Bagger (Johns Hopkins), R.M. Barnett (LBNL), C.H. Chen (UC Davis), G. Cleaver (OSU), B. Dobrescu (BU), M. Drees (Wisconsin), J.F. Gunion (UC Davis), G.L. Kane (Michigan), B. Kayser (NSF), C. Kolda (IAS), J. Lykken (FNAL), S.P. Martin (Michigan), T. Moroi (LBNL), S. Mrenna (Argonne), M. Nojiri (KEK), D. Pierce (SLAC), X. Tata (Hawaii), S. Thomas (SLAC), J.D. Wells (SLAC), B. Wright (North Carolina), Y. Yamada (Wisconsin) ABSTRACT Spacetime supersymmetry appears to be a fundamental in- gredient of superstring theory. We provide a mini-guide to some of the possible manifesta- tions of weak-scale supersymmetry. For each of six scenarios These motivations say nothing about the scale at which nature we provide might be supersymmetric. Indeed, there are additional motiva- tions for weak-scale supersymmetry. a brief description of the theoretical underpinnings, Incorporation of supersymmetry into the SM leads to a so- the adjustable parameters, lution of the gauge hierarchy problem. Namely, quadratic divergences in loop corrections to the Higgs boson mass a qualitative description of the associated phenomenology at future colliders, will cancel between fermionic and bosonic loops. This mechanism works only if the superpartner particle masses comments on how to simulate each scenario with existing are roughly of order or less than the weak scale. event generators. There exists an experimental hint: the three gauge cou- plings can unify at the Grand Uni®cation scale if there ex- I. INTRODUCTION ist weak-scale supersymmetric particles, with a desert be- The Standard Model (SM) is a theory of spin- 1 matter tween the weak scale and the GUT scale. -
Quantum Field Theory*
Quantum Field Theory y Frank Wilczek Institute for Advanced Study, School of Natural Science, Olden Lane, Princeton, NJ 08540 I discuss the general principles underlying quantum eld theory, and attempt to identify its most profound consequences. The deep est of these consequences result from the in nite number of degrees of freedom invoked to implement lo cality.Imention a few of its most striking successes, b oth achieved and prosp ective. Possible limitation s of quantum eld theory are viewed in the light of its history. I. SURVEY Quantum eld theory is the framework in which the regnant theories of the electroweak and strong interactions, which together form the Standard Mo del, are formulated. Quantum electro dynamics (QED), b esides providing a com- plete foundation for atomic physics and chemistry, has supp orted calculations of physical quantities with unparalleled precision. The exp erimentally measured value of the magnetic dip ole moment of the muon, 11 (g 2) = 233 184 600 (1680) 10 ; (1) exp: for example, should b e compared with the theoretical prediction 11 (g 2) = 233 183 478 (308) 10 : (2) theor: In quantum chromo dynamics (QCD) we cannot, for the forseeable future, aspire to to comparable accuracy.Yet QCD provides di erent, and at least equally impressive, evidence for the validity of the basic principles of quantum eld theory. Indeed, b ecause in QCD the interactions are stronger, QCD manifests a wider variety of phenomena characteristic of quantum eld theory. These include esp ecially running of the e ective coupling with distance or energy scale and the phenomenon of con nement. -
Theoretical and Experimental Aspects of the Higgs Mechanism in the Standard Model and Beyond Alessandra Edda Baas University of Massachusetts Amherst
University of Massachusetts Amherst ScholarWorks@UMass Amherst Masters Theses 1911 - February 2014 2010 Theoretical and Experimental Aspects of the Higgs Mechanism in the Standard Model and Beyond Alessandra Edda Baas University of Massachusetts Amherst Follow this and additional works at: https://scholarworks.umass.edu/theses Part of the Physics Commons Baas, Alessandra Edda, "Theoretical and Experimental Aspects of the Higgs Mechanism in the Standard Model and Beyond" (2010). Masters Theses 1911 - February 2014. 503. Retrieved from https://scholarworks.umass.edu/theses/503 This thesis is brought to you for free and open access by ScholarWorks@UMass Amherst. It has been accepted for inclusion in Masters Theses 1911 - February 2014 by an authorized administrator of ScholarWorks@UMass Amherst. For more information, please contact [email protected]. THEORETICAL AND EXPERIMENTAL ASPECTS OF THE HIGGS MECHANISM IN THE STANDARD MODEL AND BEYOND A Thesis Presented by ALESSANDRA EDDA BAAS Submitted to the Graduate School of the University of Massachusetts Amherst in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE September 2010 Department of Physics © Copyright by Alessandra Edda Baas 2010 All Rights Reserved THEORETICAL AND EXPERIMENTAL ASPECTS OF THE HIGGS MECHANISM IN THE STANDARD MODEL AND BEYOND A Thesis Presented by ALESSANDRA EDDA BAAS Approved as to style and content by: Eugene Golowich, Chair Benjamin Brau, Member Donald Candela, Department Chair Department of Physics To my loving parents. ACKNOWLEDGMENTS Writing a Thesis is never possible without the help of many people. The greatest gratitude goes to my supervisor, Prof. Eugene Golowich who gave my the opportunity of working with him this year. -
Coupling Constant Unification in Extensions of Standard Model
Coupling Constant Unification in Extensions of Standard Model Ling-Fong Li, and Feng Wu Department of Physics, Carnegie Mellon University, Pittsburgh, PA 15213 May 28, 2018 Abstract Unification of electromagnetic, weak, and strong coupling con- stants is studied in the extension of standard model with additional fermions and scalars. It is remarkable that this unification in the su- persymmetric extension of standard model yields a value of Weinberg angle which agrees very well with experiments. We discuss the other possibilities which can also give same result. One of the attractive features of the Grand Unified Theory is the con- arXiv:hep-ph/0304238v2 3 Jun 2003 vergence of the electromagnetic, weak and strong coupling constants at high energies and the prediction of the Weinberg angle[1],[3]. This lends a strong support to the supersymmetric extension of the Standard Model. This is because the Standard Model without the supersymmetry, the extrapolation of 3 coupling constants from the values measured at low energies to unifi- cation scale do not intercept at a single point while in the supersymmetric extension, the presence of additional particles, produces the convergence of coupling constants elegantly[4], or equivalently the prediction of the Wein- berg angle agrees with the experimental measurement very well[5]. This has become one of the cornerstone for believing the supersymmetric Standard 1 Model and the experimental search for the supersymmetry will be one of the main focus in the next round of new accelerators. In this paper we will explore the general possibilities of getting coupling constants unification by adding extra particles to the Standard Model[2] to see how unique is the Supersymmetric Standard Model in this respect[?]. -
The Algebra of Grand Unified Theories
The Algebra of Grand Unified Theories John Baez and John Huerta Department of Mathematics University of California Riverside, CA 92521 USA May 4, 2010 Abstract The Standard Model is the best tested and most widely accepted theory of elementary particles we have today. It may seem complicated and arbitrary, but it has hidden patterns that are revealed by the relationship between three ‘grand unified theories’: theories that unify forces and particles by extend- ing the Standard Model symmetry group U(1) × SU(2) × SU(3) to a larger group. These three are Georgi and Glashow’s SU(5) theory, Georgi’s theory based on the group Spin(10), and the Pati–Salam model based on the group SU(2)×SU(2)×SU(4). In this expository account for mathematicians, we ex- plain only the portion of these theories that involves finite-dimensional group representations. This allows us to reduce the prerequisites to a bare minimum while still giving a taste of the profound puzzles that physicists are struggling to solve. 1 Introduction The Standard Model of particle physics is one of the greatest triumphs of physics. This theory is our best attempt to describe all the particles and all the forces of nature... except gravity. It does a great job of fitting experiments we can do in the lab. But physicists are dissatisfied with it. There are three main reasons. First, it leaves out gravity: that force is described by Einstein’s theory of general relativity, arXiv:0904.1556v2 [hep-th] 1 May 2010 which has not yet been reconciled with the Standard Model. -
– 1– LEPTOQUARK QUANTUM NUMBERS Revised September
{1{ LEPTOQUARK QUANTUM NUMBERS Revised September 2005 by M. Tanabashi (Tohoku University). Leptoquarks are particles carrying both baryon number (B) and lepton number (L). They are expected to exist in various extensions of the Standard Model (SM). The possible quantum numbers of leptoquark states can be restricted by assuming that their direct interactions with the ordinary SM fermions are dimensionless and invariant under the SM gauge group. Table 1 shows the list of all possible quantum numbers with this assumption [1]. The columns of SU(3)C,SU(2)W,andU(1)Y in Table 1 indicate the QCD representation, the weak isospin representation, and the weak hypercharge, respectively. The spin of a leptoquark state is taken to be 1 (vector leptoquark) or 0 (scalar leptoquark). Table 1: Possible leptoquarks and their quan- tum numbers. Spin 3B + L SU(3)c SU(2)W U(1)Y Allowed coupling c c 0 −2 311¯ /3¯qL`Loru ¯ReR c 0 −2 314¯ /3 d¯ReR c 0−2331¯ /3¯qL`L cµ c µ 1−2325¯ /6¯qLγeRor d¯Rγ `L cµ 1 −2 32¯ −1/6¯uRγ`L 00327/6¯qLeRoru ¯R`L 00321/6 d¯R`L µ µ 10312/3¯qLγ`Lor d¯Rγ eR µ 10315/3¯uRγeR µ 10332/3¯qLγ`L If we do not require leptoquark states to couple directly with SM fermions, different assignments of quantum numbers become possible [2,3]. The Pati-Salam model [4] is an example predicting the existence of a leptoquark state. In this model a vector lepto- quark appears at the scale where the Pati-Salam SU(4) “color” gauge group breaks into the familiar QCD SU(3)C group (or CITATION: S. -
Supersymmetry Breaking and Inflation from Higher Curvature
Prepared for submission to JHEP Supersymmetry Breaking and Inflation from Higher Curvature Supergravity I. Dalianisa, F. Farakosb, A. Kehagiasa;c, A. Riottoc and R. von Ungeb aPhysics Division, National Technical University of Athens, 15780 Zografou Campus, Athens, Greece bInstitute for Theoretical Physics, Masaryk University, 611 37 Brno, Czech Republic cDepartment of Theoretical Physics and Center for Astroparticle Physics (CAP) 24 quai E. Ansermet, CH-1211 Geneva 4, Switzerland E-mail: [email protected], [email protected], [email protected], [email protected], [email protected] Abstract: The generic embedding of the R + R2 higher curvature theory into old- minimal supergravity leads to models with rich vacuum structure in addition to its well-known inflationary properties. When the model enjoys an exact R-symmetry, there is an inflationary phase with a single supersymmetric Minkowski vacuum. This appears to be a special case of a more generic set-up, which in principle may include R- symmetry violating terms which are still of pure supergravity origin. By including the latter terms, we find new supersymmetry breaking vacua compatible with single-field inflationary trajectories. We discuss explicitly two such models and we illustrate how arXiv:1409.8299v2 [hep-th] 22 Jan 2015 the inflaton is driven towards the supersymmetry breaking vacuum after the inflationary phase. In these models the gravitino mass is of the same order as the inflaton mass. Therefore, pure higher curvature supergravity may not only accommodate the proper inflaton field, but it may also provide the appropriate hidden sector for supersymmetry breaking after inflation has ended. -
TASI 2008 Lectures: Introduction to Supersymmetry And
TASI 2008 Lectures: Introduction to Supersymmetry and Supersymmetry Breaking Yuri Shirman Department of Physics and Astronomy University of California, Irvine, CA 92697. [email protected] Abstract These lectures, presented at TASI 08 school, provide an introduction to supersymmetry and supersymmetry breaking. We present basic formalism of supersymmetry, super- symmetric non-renormalization theorems, and summarize non-perturbative dynamics of supersymmetric QCD. We then turn to discussion of tree level, non-perturbative, and metastable supersymmetry breaking. We introduce Minimal Supersymmetric Standard Model and discuss soft parameters in the Lagrangian. Finally we discuss several mech- anisms for communicating the supersymmetry breaking between the hidden and visible sectors. arXiv:0907.0039v1 [hep-ph] 1 Jul 2009 Contents 1 Introduction 2 1.1 Motivation..................................... 2 1.2 Weylfermions................................... 4 1.3 Afirstlookatsupersymmetry . .. 5 2 Constructing supersymmetric Lagrangians 6 2.1 Wess-ZuminoModel ............................... 6 2.2 Superfieldformalism .............................. 8 2.3 VectorSuperfield ................................. 12 2.4 Supersymmetric U(1)gaugetheory ....................... 13 2.5 Non-abeliangaugetheory . .. 15 3 Non-renormalization theorems 16 3.1 R-symmetry.................................... 17 3.2 Superpotentialterms . .. .. .. 17 3.3 Gaugecouplingrenormalization . ..... 19 3.4 D-termrenormalization. ... 20 4 Non-perturbative dynamics in SUSY QCD 20 4.1 Affleck-Dine-Seiberg -
Critical Coupling for Dynamical Chiral-Symmetry Breaking with an Infrared Finite Gluon Propagator *
BR9838528 Instituto de Fisica Teorica IFT Universidade Estadual Paulista November/96 IFT-P.050/96 Critical coupling for dynamical chiral-symmetry breaking with an infrared finite gluon propagator * A. A. Natale and P. S. Rodrigues da Silva Instituto de Fisica Teorica Universidade Estadual Paulista Rua Pamplona 145 01405-900 - Sao Paulo, S.P. Brazil *To appear in Phys. Lett. B t 2 9-04 Critical Coupling for Dynamical Chiral-Symmetry Breaking with an Infrared Finite Gluon Propagator A. A. Natale l and P. S. Rodrigues da Silva 2 •r Instituto de Fisica Teorica, Universidade Estadual Paulista Rua Pamplona, 145, 01405-900, Sao Paulo, SP Brazil Abstract We compute the critical coupling constant for the dynamical chiral- symmetry breaking in a model of quantum chromodynamics, solving numer- ically the quark self-energy using infrared finite gluon propagators found as solutions of the Schwinger-Dyson equation for the gluon, and one gluon prop- agator determined in numerical lattice simulations. The gluon mass scale screens the force responsible for the chiral breaking, and the transition occurs only for a larger critical coupling constant than the one obtained with the perturbative propagator. The critical coupling shows a great sensibility to the gluon mass scale variation, as well as to the functional form of the gluon propagator. 'e-mail: [email protected] 2e-mail: [email protected] 1 Introduction The idea that quarks obtain effective masses as a result of a dynamical breakdown of chiral symmetry (DBCS) has received a great deal of attention in the last years [1, 2]. One of the most common methods used to study the quark mass generation is to look for solutions of the Schwinger-Dyson equation for the fermionic propagator. -
The Higgs Boson and the Cosmology of the Early Universe Mikhail Shaposhnikov Blois 2018
The Higgs Boson and the Cosmology of the Early Universe Mikhail Shaposhnikov Blois 2018 Rencontres de Blois, June 4, 2018 – p. 1 Almost 6 years with the Higgs boson: July 4, 2012, Higgs at ATLAS and CMS 3500 ATLAS Data Sig+Bkg Fit (m =126.5 GeV) 3000 H Bkg (4th order polynomial) 2500 Events / 2 GeV 2000 1500 s=7 TeV, ∫Ldt=4.8fb-1 1000 s=8 TeV, ∫Ldt=5.9fb-1 γγ→ 500 H (a) 200100 110 120 130 140 150 160 100 0 -100 Events - Bkg (b) -200 100 110 120 130 140 150 160 Data S/B Weighted 100 Sig+Bkg Fit (m =126.5 GeV) H Bkg (4th order polynomial) 80 weights / 2 GeV Σ 60 40 20 (c) 8100 110 120 130 140 150 160 4 0 -4 (d) -8 Σ weights - Bkg 100 110 120 130 140 150 160 m γγ [GeV] Rencontres de Blois, June 4, 2018 – p. 2 What did we learn from the Higgs discovery for particle physics? Rencontres de Blois, June 4, 2018 – p. 3 The ideas of the authors of the BEH mechanism were right Rencontres de Blois, June 4, 2018 – p. 4 The Standard Model is now complete Rencontres de Blois, June 4, 2018 – p. 5 126 125 U U U GeV Triumph of the SM in particle physics No significant deviations from the SM have been observed Rencontres de Blois, June 4, 2018 – p. 6 126 125 U U U GeV Triumph of the SM in particle physics No significant deviations from the SM have been observed The masses of the top quark and of the Higgs boson, the Nature has chosen, make the SM a self-consistent effective field theory all the way up to the quantum gravity Planck scale MP . -
Masse Des Neutrinos Et Physique Au-Delà Du Modèle Standard
œa UNIVERSITE PARIS-SUD XI THESE Spécialité: PHYSIQUE THÉORIQUE Présentée pour obtenir le grade de Docteur de l'Université Paris XI par Pierre Hosteins Sujet: Masse des Neutrinos et Physique au-delà du Modèle Standard Soutenue le 10 Septembre 2007 devant la commission d'examen: MM. Asmaa Abada, Sacha Davidson, Emilian Dudas, rapporteur, Ulrich Ellwanger, président, Belen Gavela, Thomas Hambye, rapporteur, Stéphane Lavignac, directeur de thèse. 2 Remerciements : Un travail de thèse est un travail de longue haleine, au cours duquel se produisent inévitablement beaucoup de rencontres, de collaborations, d'échanges... Voila pourquoi, sans doute, il me semble que la liste des personnes a qui je suis redevable est devenue aussi longue ! Tâchons cependant de remercier chacun comme il le mérite. En relisant ce manuscrit je ne peux m'empêcher de penser a Stéphane Lavignac, que je me dois de remercier pour avoir accepté d'encadrer mon travail de thèse et qui m'a toujours apporté le soutien et les explications nécessaires, avec une patience admirable. Sa grande rigueur d'analyse et sa minutie m'offrent un exemple que je m'évertuerai à suivre avec la plus grande application. Ces travaux n'auraient pas pu voir le jour non plus sans mes autres collaborateurs que sont Carlos Savoy, Julien Welzel, Micaela Oertel, Aldo Deandrea, Asmâa Abada et François-Xavier Josse-Michaux, qui ont toujours été disponibles et avec qui j'ai eu un plaisir certain a travailler. C'est avec gratitude que je remercie Asmâa pour tous les conseils et recommandations qu'elle n'a cessé de me fournir tout au long de mes études au sein de l'Université Paris XL Au cours de ces trois années de travail dans le domaine de la Physique Au-delà de Modèle Standard, j'ai bénéficié du contact de toute la communauté des théoriciens de la région. -
CP Violation Beyond the Standard Model*
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS G: NUCLEAR AND PARTICLE PHYSICS J. Phys. G: Nucl. Part. Phys. 28 (2002) 345–358 PII: S0954-3899(02)30104-X CP violation beyond the standard model* GLKane1 and D D Doyle2 1 Randall Physics Laboratory, University of Michigan, Ann Arbor, MI 48109, USA 2 CPES, University of Sussex, Falmer, Brighton BN1 9QJ, UK E-mail: [email protected] Received 25 October 2001 Published 21 January 2002 Online at stacks.iop.org/JPhysG/28/345 Abstract In this paper a number of broad issues are raised about the origins of CP violation and how to test the ideas. 1. Introduction The fundamental sources of CP violation in theories of physics beyond the standard model is an important issue which has not been sufficiently studied. In this paper, we begin by discussing the possible origins of CP violation in string theory and the potential influence of its phenomenology on string theory. This naturally develops into a consideration of supersymmetry breaking, specifically the soft-breaking supersymmetric Lagrangian, Lsoft. There exist two extreme scenarios which may realistically accommodate CP violation; the first involves small soft phases and a large CKM phase, δCKM, whereas the second contains large soft phases and small δCKM. We argue that there is reasonable motivation for δCKM to be almost zero and that the latter scenario should be taken seriously. Consequently, it is appropriate to consider what CP violating mechanisms could allow for large soft phases, and hence measurements of these soft phases (which can be deduced from collider results, mixings and decays, experiments exploring the Higgs sector or from electric dipole moment values) provide some interesting phenomenological implications for physics beyond the standard model.