Gauged N=1 Supergravity and the Embedding Tensor Formalism
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Renormalization Group Flows from Holography; Supersymmetry and a C-Theorem
© 1999 International Press Adv. Theor. Math. Phys. 3 (1999) 363-417 Renormalization Group Flows from Holography; Supersymmetry and a c-Theorem D. Z. Freedmana, S. S. Gubser6, K. Pilchc and N. P. Warnerd aDepartment of Mathematics and Center for Theoretical Physics, Massachusetts Institute of Technology, Cambridge, MA 02139 b Department of Physics, Harvard University, Cambridge, MA 02138, USA c Department of Physics and Astronomy, University of Southern California, Los Angeles, CA 90089-0484, USA d Theory Division, CERN, CH-1211 Geneva 23, Switzerland Abstract We obtain first order equations that determine a super symmetric kink solution in five-dimensional Af = 8 gauged supergravity. The kink interpo- lates between an exterior anti-de Sitter region with maximal supersymme- try and an interior anti-de Sitter region with one quarter of the maximal supersymmetry. One eighth of supersymmetry is preserved by the kink as a whole. We interpret it as describing the renormalization group flow in J\f = 4 super-Yang-Mills theory broken to an Af = 1 theory by the addition of a mass term for one of the three adjoint chiral superfields. A detailed cor- respondence is obtained between fields of bulk supergravity in the interior anti-de Sitter region and composite operators of the infrared field theory. We also point out that the truncation used to find the reduced symmetry critical point can be extended to obtain a new Af = 4 gauged supergravity theory holographically dual to a sector of Af = 2 gauge theories based on quiver diagrams. e-print archive: http.y/xxx.lanl.gov/abs/hep-th/9904017 *On leave from Department of Physics and Astronomy, USC, Los Angeles, CA 90089 364 RENORMALIZATION GROUP FLOWS We consider more general kink geometries and construct a c-function that is positive and monotonic if a weak energy condition holds in the bulk gravity theory. -
On the Trace Anomaly of a Weyl Fermion in a Gauge Background
On the trace anomaly of a Weyl fermion in a gauge background Fiorenzo Bastianelli,a;b;c Matteo Broccoli,a;c aDipartimento di Fisica ed Astronomia, Universit`adi Bologna, via Irnerio 46, I-40126 Bologna, Italy bINFN, Sezione di Bologna, via Irnerio 46, I-40126 Bologna, Italy cMax-Planck-Institut f¨ur Gravitationsphysik (Albert-Einstein-Institut) Am M¨uhlenberg 1, D-14476 Golm, Germany E-mail: [email protected], [email protected] Abstract: We study the trace anomaly of a Weyl fermion in an abelian gauge background. Although the presence of the chiral anomaly implies a breakdown of gauge invariance, we find that the trace anomaly can be cast in a gauge invariant form. In particular, we find that it does not contain any odd-parity contribution proportional to the Chern-Pontryagin density, which would be allowed by the con- sistency conditions. We perform our calculations using Pauli-Villars regularization and heat kernel methods. The issue is analogous to the one recently discussed in the literature about the trace anomaly of a Weyl fermion in curved backgrounds. Keywords: Anomalies in Field and String Theories, Conformal Field Theory arXiv:1808.03489v2 [hep-th] 7 May 2019 Contents 1 Introduction1 2 Actions and symmetries3 2.1 The Weyl fermion3 2.1.1 Mass terms5 2.2 The Dirac fermion8 2.2.1 Mass terms9 3 Regulators and consistent anomalies 10 4 Anomalies 13 4.1 Chiral and trace anomalies of a Weyl fermion 13 4.1.1 PV regularization with Majorana mass 14 4.1.2 PV regularization with Dirac mass 15 4.2 Chiral and trace anomalies of a Dirac fermion 16 4.2.1 PV regularization with Dirac mass 16 4.2.2 PV regularization with Majorana mass 17 5 Conclusions 18 A Conventions 19 B The heat kernel 21 C Sample calculations 22 1 Introduction In this paper we study the trace anomaly of a chiral fermion coupled to an abelian gauge field in four dimensions. -
Solutions and Democratic Formulation of Supergravity Theories in Four Dimensions
Universidad Consejo Superior Aut´onoma de Madrid de Investigaciones Cient´ıficas Facultad de Ciencias Instituto de F´ısica Te´orica Departamento de F´ısica Te´orica IFT–UAM/CSIC Solutions and Democratic Formulation of Supergravity Theories in Four Dimensions Mechthild Hubscher¨ Madrid, May 2009 Copyright c 2009 Mechthild Hubscher.¨ Universidad Consejo Superior Aut´onoma de Madrid de Investigaciones Cient´ıficas Facultad de Ciencias Instituto de F´ısica Te´orica Departamento de F´ısica Te´orica IFT–UAM/CSIC Soluciones y Formulaci´on Democr´atica de Teor´ıas de Supergravedad en Cuatro Dimensiones Memoria de Tesis Doctoral realizada por Da Mechthild Hubscher,¨ presentada ante el Departamento de F´ısica Te´orica de la Universidad Aut´onoma de Madrid para la obtenci´on del t´ıtulo de Doctora en Ciencias. Tesis Doctoral dirigida por Dr. D. Tom´as Ort´ın Miguel, Investigador Cient´ıfico del Consejo Superior de Investigaciones Cient´ıficas, y Dr. D. Patrick Meessen, Investigador Contratado por el Consejo Superior de Investigaciones Cient´ıficas. Madrid, Mayo de 2009 Contents 1 Introduction 1 1.1 Supersymmetry, Supergravity and Superstring Theory . ....... 1 1.2 Gauged Supergravity and the p-formhierarchy . 10 1.3 Supersymmetric configurations and solutions of Supergravity ..... 18 1.4 Outlineofthisthesis............................ 23 2 Ungauged N =1, 2 Supergravity in four dimensions 25 2.1 Ungauged matter coupled N =1Supergravity. 25 2.1.1 Perturbative symmetries of the ungauged theory . ... 27 2.1.2 Non-perturbative symmetries of the ungauged theory . ..... 33 2.2 Ungauged matter coupled N =2Supergravity. 35 2.2.1 N = 2, d =4SupergravityfromStringTheory . 42 3 Gauging Supergravity and the four-dimensional tensor hierarchy 49 3.1 Theembeddingtensorformalism . -
Chiral Gauge Theories Revisited
CERN-TH/2001-031 Chiral gauge theories revisited Lectures given at the International School of Subnuclear Physics Erice, 27 August { 5 September 2000 Martin L¨uscher ∗ CERN, Theory Division CH-1211 Geneva 23, Switzerland Contents 1. Introduction 2. Chiral gauge theories & the gauge anomaly 3. The regularization problem 4. Weyl fermions from 4+1 dimensions 5. The Ginsparg–Wilson relation 6. Gauge-invariant lattice regularization of anomaly-free theories 1. Introduction A characteristic feature of the electroweak interactions is that the left- and right- handed components of the fermion fields do not couple to the gauge fields in the same way. The term chiral gauge theory is reserved for field theories of this type, while all other gauge theories (such as QCD) are referred to as vector-like, since the gauge fields only couple to vector currents in this case. At first sight the difference appears to be mathematically insignificant, but it turns out that in many respects chiral ∗ On leave from Deutsches Elektronen-Synchrotron DESY, D-22603 Hamburg, Germany 1 νµ ν e µ W W γ e Fig. 1. Feynman diagram contributing to the muon decay at two-loop order of the electroweak interactions. The triangular subdiagram in this example is potentially anomalous and must be treated with care to ensure that gauge invariance is preserved. gauge theories are much more complicated. Their definition beyond the classical level, for example, is already highly non-trivial and it is in general extremely difficult to obtain any solid information about their non-perturbative properties. 1.1 Anomalies Most of the peculiarities in chiral gauge theories are related to the fact that the gauge symmetry tends to be violated by quantum effects. -
UNIVERSITY of CALIFORNIA Los Angeles Conformal Defects In
UNIVERSITY OF CALIFORNIA Los Angeles Conformal Defects in Gauged Supergravity A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Physics by Matteo Vicino 2020 c Copyright by Matteo Vicino 2020 ABSTRACT OF THE DISSERTATION Conformal Defects in Gauged Supergravity by Matteo Vicino Doctor of Philosophy in Physics University of California, Los Angeles, 2020 Professor Michael Gutperle, Chair In this dissertation, we explore 1/2-BPS conformal defects that are holographically realized as a warped product of anti-de Sitter spacetime and a circle in gauged supergravity. These solutions can be obtained as the double analytic continuation of BPS black holes with hy- perbolic horizons. Observables including the expectation value of the defect and one-point functions of fields in the presence of the defect are calculated. In Chapter 1, we present a brief review of the AdS/CFT correspondence and its super- gravity approximation together with an introduction to conformal defects. In Chapter 2, we construct a singular spacetime in pure D = 4;N = 2 gauged supergravity dual to a 1/2-BPS conformal line defect. In Chapter 3, we show that the coupling of vector multiplets to the previous solution is capable of removing the singularity and present several examples. In Chapter 4, we construct solutions in D = 5;N = 4 gauged supergravity dual to 1/2-BPS surface operators in N = 2 superconformal field theories. ii The dissertation of Matteo Vicino is approved. Thomas Dumitrescu Eric D'Hoker Per Kraus Michael Gutperle, Committee Chair University of California, Los Angeles 2020 iii Table of Contents 1 Introduction :::::::::::::::::::::::::::::::::::::: 1 1.1 The AdS/CFT Correspondence . -
Nonperturbative Definition of the Standard Models
PHYSICAL REVIEW RESEARCH 2, 023356 (2020) Nonperturbative definition of the standard models Juven Wang 1,2,* and Xiao-Gang Wen3 1School of Natural Sciences, Institute for Advanced Study, Princeton, New Jersey 08540, USA 2Center of Mathematical Sciences and Applications, Harvard University, Cambridge, Massachusetts 02138, USA 3Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA (Received 14 June 2019; accepted 21 May 2020; published 17 June 2020) The standard models contain chiral fermions coupled to gauge theories. It has been a longstanding problem to give such gauged chiral fermion theories a quantum nonperturbative definition. By classification of quantum anomalies (including perturbative local anomalies and nonperturbative global anomalies) and symmetric interacting invertible topological orders via a mathematical cobordism theorem for differentiable and triangulable manifolds, and by the existence of a symmetric gapped boundary (designed for the mirror sector) on the trivial symmetric invertible topological orders, we propose that Spin(10) chiral fermion theories with Weyl fermions in 16-dimensional spinor representations can be defined on a 3 + 1D lattice without fermion doubling, and subsequently dynamically gauged to be a Spin(10) chiral gauge theory. As a result, the standard models from the 16n-chiral fermion SO(10) grand unification can be defined nonperturbatively via a 3 + 1D local lattice model of bosons or qubits. Furthermore, we propose that standard models from the 15n-chiral fermion -
U(1) Gauge Extensions of the Standard Model
U(1) Gauge Extensions of the Standard Model Ernest Ma Physics and Astronomy Department University of California Riverside, CA 92521, USA U(1) Gauge Extensions of the Standard Model (int08) back to start 1 Contents • Anomaly Freedom of the Standard Model • B − L • Le − Lµ and B − 3Lτ • U(1)Σ • Supersymmetric U(1)X • Some Remarks U(1) Gauge Extensions of the Standard Model (int08) back to start 2 Anomaly Freedom of the Standard Model Gauge Group: SU(3)C × SU((2)L × U(1)Y . Consider the fermion multiplets: (u, d)L ∼ (3, 2, n1), uR ∼ (3, 1, n2), dR ∼ (3, 1, n3), (ν, e)L ∼ (1, 2, n4), eR ∼ (1, 1, n5). Bouchiat/Iliopolous/Meyer(1972): The SM with n1 = 1/6, n2 = 2/3, n3 = −1/3, n4 = −1/2, n5 = −1, is free of axial-vector anomalies, i.e. 2 [SU(3)] U(1)Y : 2n1 − n2 − n3 = 0. 2 [SU(2)] U(1)Y : 3n1 + n4 = 0. 3 3 3 3 3 3 [U(1)Y ] : 6n1 − 3n2 − 3n3 + 2n4 − n5 = 0. U(1) Gauge Extensions of the Standard Model (int08) back to start 3 It is also free of the mixed gravitational-gauge anomaly, U(1)Y : 6n1 − 3n2 − 3n3 + 2n4 − n5 = 0. Geng/Marshak(1989), Minahan/Ramond/Warner(1990) : Above 4 equations ⇒ n1(4n1 − n2)(2n1 + n2) = 0. n2 = 4n1 ⇒ SM; n2 = −2n1 ⇒ SM (uR ↔ dR); n1 = 0 ⇒ n4 = n5 = n2 + n3 = 0. Here eR ∼ (1, 1, 0) may be dropped. (u, d)L, (ν, e)L have charges (1/2, −1/2) and (uR, dR) have charges (n2, −n2). -
Introduction to Supergravity
Introduction to Supergravity Lectures presented by Henning Samtleben at the 13th Saalburg School on Fundamentals and New Methods in Theoretical Physics, September 3 { 14, 2007 typed by Martin Ammon and Cornelius Schmidt-Colinet ||| 1 Contents 1 Introduction 3 2 N = 1 supergravity in D = 4 dimensions 4 2.1 General aspects . 4 2.2 Gauging a global symmetry . 5 2.3 The vielbein formalism . 6 2.4 The Palatini action . 9 2.5 The supersymmetric action . 9 2.6 Results . 14 3 Extended supergravity in D = 4 dimensions 16 3.1 Matter couplings in N = 1 supergravity . 16 3.2 Extended supergravity in D = 4 dimensions . 17 4 Extended supergravity in higher Dimensions 18 4.1 Spinors in higher dimensions . 18 4.2 Eleven-dimensional supergravity . 20 4.3 Kaluza-Klein supergravity . 22 4.4 N = 8 supergravity in D = 4 dimensions . 26 A Variation of the Palatini action 27 2 1 Introduction There are several reasons to consider the combination of supersymmetry and gravitation. The foremost is that if supersymmetry turns out to be realized at all in nature, then it must eventually appear in the context of gravity. As is characteristic for supersymmetry, its presence is likely to improve the quantum behavior of the theory, particularly interesting in the context of gravity, a notoriously non-renormalizable theory. Indeed, in supergravity divergences are typically delayed to higher loop orders, and to date it is still not ruled out that the maximally supersymmetric extension of four-dimensional Einstein gravity might eventually be a finite theory of quantum gravity | only recently very tempting indications in this direction have been unvealed. -
Green-Schwarz Anomaly Cancellation
Green-Schwarz anomaly cancellation Paolo Di Vecchia Niels Bohr Instituttet, Copenhagen and Nordita, Stockholm Collège de France, 05.03.10 Paolo Di Vecchia (NBI+NO) GS anomaly cancellation Collège de France, 05.03.10 1 / 30 Plan of the talk 1 Introduction 2 A quick look at the abelian axial anomaly 3 Few words on forms 4 Anomaly cancellation in type IIB superstring theory 5 Anomaly cancellation in type I superstring 6 Conclusions Paolo Di Vecchia (NBI+NO) GS anomaly cancellation Collège de France, 05.03.10 2 / 30 Introduction I The theory of general relativity for gravity was formulated by Einstein in 1915. I It is a four-dimensional theory that extends the theory of special relativity. I While special relativity is invariant under the transformations of the Lorentz group, general relativity is invariant under an arbitrary change of coordinates. I In the twenties it was proposed by Theodor Kaluza and Oskar Klein to unify electromagnetism with gravity by starting from general relativity in a five-dimensional space-time and compactify the extra-dimension on a small circle. I In this way one obtains general relativity in four dimensions, a vector gauge field satisfying the Maxwell equations and a scalar. I This idea of extra dimensions was not pursued in the years after. I In the sixties and seventies, when I started to work in the physics of the elementary particles, everybody was strictly working in four dimensions. Paolo Di Vecchia (NBI+NO) GS anomaly cancellation Collège de France, 05.03.10 3 / 30 I Also the dual resonance model, being a model for hadrons, was obviously formulated in four dimensions. -
Anomaly-Free Supergravities in Six Dimensions
Anomaly-Free Supergravities in Six Dimensions Ph.D. Thesis arXiv:hep-th/0611133v1 12 Nov 2006 Spyros D. Avramis National Technical University of Athens School of Applied Mathematics and Natural Sciences Department of Physics Spyros D. Avramis Anomaly-Free Supergravities in Six Dimensions Dissertation submitted to the Department of Physics of the National Technical University of Athens in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Physics. Thesis Advisor: Alex Kehagias Thesis Committee: Alex Kehagias Elias Kiritsis George Zoupanos K. Anagnostopoulos A.B. Lahanas E. Papantonopoulos N.D. Tracas Athens, February 2006 Abstract This thesis reviews minimal N = 2 chiral supergravities coupled to matter in six dimensions with emphasis on anomaly cancellation. In general, six-dimensional chiral supergravities suffer from gravitational, gauge and mixed anomalies which, being associated with the breakdown of local gauge symmetries, render the theories inconsistent at the quantum level. Consistency of the theory is restored if the anomalies of the theory cancel via the Green-Schwarz mechanism or generalizations thereof, in a similar manner as in the case of ten-dimensional N = 1 supergravi- ties. The anomaly cancellation conditions translate into a certain set of constraints for the gauge group of the theory as well as on its matter content. For the case of ungauged theories these constraints admit numerous solutions but, in the case of gauged theories, the allowed solutions are remarkably few. In this thesis, we examine these anomaly cancellation conditions in detail and we present all solutions to these conditions under certain restrictions on the allowed gauge groups and representations, imposed for practical reasons. -
Anomalies and the Standard Model of Particle Physics
Anomalies and the Standard Model of Particle Physics Nakarin Lohitsiri Supervisor: Professor David Tong Department of Applied Mathematics and Theoretical Physics University of Cambridge This dissertation is submitted for the degree of Doctor of Philosophy Trinity College August 2020 For my parents Declaration This dissertation is based on original research done by the author while he was a graduate student at the Department of Applied Mathematics and Theoretical Physics, University of Cambridge, between October 2016 and August 2020. The material in Chapters2 and5 is based on the work done by the author under the supervision of David Tong and has been partly published in References [97, 96], while Chapters3 and4 are based on research done in collaboration with Joe Davighi, part of which is published in References [53, 52]. Except for part of Chapter3 that has been previously submitted for a degree of doctor of philosophy by Joe Davighi at the University of Cambridge, no other part of this work has been submitted, or is being concurrently submitted, for a degree or other qualification at the University of Cambridge or any other university or similar institution. Nakarin Lohitsiri August 2020 Anomalies and the Standard Model of Particle Physics Nakarin Lohitsiri This dissertation aims to study quantum anomalies and some other aspects of the Standard Model of Particle physics. In any quantum gauge field theory, anomalies place a very restrictive condition on the matter content and the dynamics. The former is due to the cancellation of gauge anomalies while ’t Hooft anomaly matching constraints produce the latter. As the Standard Model, which is our most fundamental and most accurate description of particle physics, is constructed as a gauge field theory, it is also subject to these anomalies. -
Gauge Theory
Preprint typeset in JHEP style - HYPER VERSION 2018 Gauge Theory David Tong Department of Applied Mathematics and Theoretical Physics, Centre for Mathematical Sciences, Wilberforce Road, Cambridge, CB3 OBA, UK http://www.damtp.cam.ac.uk/user/tong/gaugetheory.html [email protected] Contents 0. Introduction 1 1. Topics in Electromagnetism 3 1.1 Magnetic Monopoles 3 1.1.1 Dirac Quantisation 4 1.1.2 A Patchwork of Gauge Fields 6 1.1.3 Monopoles and Angular Momentum 8 1.2 The Theta Term 10 1.2.1 The Topological Insulator 11 1.2.2 A Mirage Monopole 14 1.2.3 The Witten Effect 16 1.2.4 Why θ is Periodic 18 1.2.5 Parity, Time-Reversal and θ = π 21 1.3 Further Reading 22 2. Yang-Mills Theory 26 2.1 Introducing Yang-Mills 26 2.1.1 The Action 29 2.1.2 Gauge Symmetry 31 2.1.3 Wilson Lines and Wilson Loops 33 2.2 The Theta Term 38 2.2.1 Canonical Quantisation of Yang-Mills 40 2.2.2 The Wavefunction and the Chern-Simons Functional 42 2.2.3 Analogies From Quantum Mechanics 47 2.3 Instantons 51 2.3.1 The Self-Dual Yang-Mills Equations 52 2.3.2 Tunnelling: Another Quantum Mechanics Analogy 56 2.3.3 Instanton Contributions to the Path Integral 58 2.4 The Flow to Strong Coupling 61 2.4.1 Anti-Screening and Paramagnetism 65 2.4.2 Computing the Beta Function 67 2.5 Electric Probes 74 2.5.1 Coulomb vs Confining 74 2.5.2 An Analogy: Flux Lines in a Superconductor 78 { 1 { 2.5.3 Wilson Loops Revisited 85 2.6 Magnetic Probes 88 2.6.1 't Hooft Lines 89 2.6.2 SU(N) vs SU(N)=ZN 92 2.6.3 What is the Gauge Group of the Standard Model? 97 2.7 Dynamical Matter 99 2.7.1 The Beta Function Revisited 100 2.7.2 The Infra-Red Phases of QCD-like Theories 102 2.7.3 The Higgs vs Confining Phase 105 2.8 't Hooft-Polyakov Monopoles 109 2.8.1 Monopole Solutions 112 2.8.2 The Witten Effect Again 114 2.9 Further Reading 115 3.