Instituto De Física Teórica UAM-CSIC

Total Page:16

File Type:pdf, Size:1020Kb

Instituto De Física Teórica UAM-CSIC Instituto de Física Teórica UAM-CSIC UNIVERSIDAD AUTÓNOMA DE MADRID TESIS DOCTORAL Anomalous Transport in Hydrodynamics and Gauge/Gravity Duality Out of Equilibrium Autor: Director: Jorge FERNÁNDEZ PENDÁS Dr. Karl LANDSTEINER 9 de octubre de 2019 iii Many things can happen in four years, but none of them has as much of an impact on you as the people you meet along the way. I would like to start thanking Miguel Ángel Ramos Osorio, who acted as a guide in the first days of my scientific career. Miguel Ángel, I learned from you the impor- tance of professional honesty and excellence. You left us too early, but will always be remembered. Much of this thesis would not be the same without my supervisor, Karl Landsteiner. My way of understanding physics has been forever altered by our dis- cussions. Karl, I know how lucky I am by having you as my advisor. Your patience, respect and trust are a happy anomaly. My scientific brother, Christian Copetti, has been the best possible teammate. As in a doubles game, one stayed in the net as the other served. I hope I have contributed to your growth as much as you have contributed to mine. I would also like to thank all the rest of my collaborators. Yan Liu and Matthias Kaminski deserve a special mention because they have also been international ref- erees for this thesis. Along with Matthias, I should also thank all the people from Tuscaloosa that made my stay one of the most interesting periods of the PhD. An- gela, Casey, Jana, Markus, Roshan... thank you for your hospitality and considera- tion. All the people that have been members of the IFT in the last years are responsible for creating the right atmosphere for this thesis to be completed. However, I would like to especially thank Thomas Biekötter, Iñaki Lara, Javier Martín, Diego Medrano, Sebastián Montes, Javier Rodríguez-Laguna, Sara Saa and Nadir Samos for your friendship and the long conversations... about everything. Good luck to everyone! I am eternally grateful to Francisco Fernández and Diego Gutiérrez for their friendship during our shared year in Madrid and their capability to make those stressful times fun. I must confess that during the last four years I have missed those lunches at Plaza Mayor. Another close friend that shared some months with me in Madrid, although our friendship started long before, is Fafa. Our mutual support during times of uncer- tainty stays with us forever. With him, I would also like to mention the rest of my non-Physics-related friends. You are too many to be included here, but achieve- ments like this can only be made with a solid network of support. My family has taught me so many things it is impossible to sum them all up here. Your generosity and commitment have always shined a light on my path, and they are an endless source of confidence and happiness. I love you so much! I have saved the last words of gratitude for my partner. Paula, you have been understanding and supporting me for almost nine years now, and I can safely say that your contribution to this thesis is almost as important as mine. Your strength and enthusiasm are my inspiration every day. Russian physicist Lev Landau once said, “It is important to do everything with passion, it embellishes life enormously”. My life is certainly more beautiful with you. Thank you! Danke schön! Grazie mille! ""! ¡Muchas gracias! v Summary Anomalous transport has been a topic of great interest in the last decade. New dissi- pationless contributions to the charge and energy currents arise due to the existence of a chiral anomaly, which is the breaking at the quantum level of the chiral symme- try. Those transport phenomena are studied using holography because they are ex- pected to be important in experimental setups at strong coupling. Moreover, we know that the anomaly has the same value independently of the energy scale, so we can expect to extract the universal behavior of anomalous transport by performing our computations in the nonperturbative regime. Therefore, in this thesis we use the AdS/CFT correspondence to study different features of anomaly induced transport. Let us now summarize the content of each chapter. In Chapter1, anomalous transport is presented in relation to the experimental setups in which it appears and the content of the other chapters is summarized. In Chapter2, all the theoretical background required for this thesis is introduced. In particular, the chapter includes sections for anomalies, relativistic hydrodynamics, linear response theory and holography. Both Chapters1 and2 serve as an introduc- tion. In Chapter3, we explore how symmetries in gravity can be exploited to simplify the computation of anomalous transport coefficients. In holography, the radial coor- dinate of AdS is dual to an energy scale for the field theory. Therefore, holographic renormalization group flows can be better understood through radially conserved charges. It has been shown in previous works that the bulk gauge and diffeomor- phism symmetries can be used to find conserved quantities associated to the charge and heat currents. However, the application to anomalous transport is cumbersome, because Chern-Simons terms in the action break gauge invariance and, moreover, the gravitational Chern-Simons involves a higher number of derivatives. Neverthe- less, we show that conservation laws can still be derived and they allow to obtain the field theory observables in terms of quantities evaluated at the horizon. In Chapter4, we study a case in which it becomes evident that the construction of membrane currents from Chapter3 is necessary to compute the charge and energy currents. Translation symmetry breaking is introduced through the use of spatially linear scalar field backgrounds and a further coupling between the scalars and an electromagnetic field is included to produce disorder on the charged sector. The result we find is that the electric conductivity can vanish for certain values of the translation symmetry breaking couplings, and the chiral magnetic and chiral vor- tical conductivities are not affected by the inclusion of momentum relaxation and charged disorder. This is to be expected from the dissipationless nature of anoma- lous transport. In Chapter5, we study the holographic model of Weyl semimetals that was pro- posed by our research group some months before the beginning of this PhD. Its vi main feature is the appearance of a topological quantum phase transition between a topological phase with nonvanishing anomalous Hall effect and a trivial phase without such effect. Our work has focused on studying the universality of this phase transition as a function of the free parameters of the model and then extending the computation of the anomalous Hall effect in the vector current to the analogous con- tribution in the axial current. As a result, we find that the phase transition appears for a large region of parameter space, and the axial Hall effect can be found to give the expected value once a renormalization of the external axial fields due to their coupling to the scalars is considered. In Chapter6, we extend the study of anomalous transport to out of equilibrium setups. In order to do that, we use generalized Vaidya metrics with momentum relaxation to induce sudden changes in the energy and charge of the system. As a result, we find that the chiral magnetic effect presents a significantly large equilibra- tion time that depends on the length of the Vaidya quench and the momentum re- laxation parameter. We expect this to give some hints on the phenomenology of the quark-gluon plasma produced in heavy ion collisions. In particular, we propose an explanation of why the experimental results from the RHIC collider in Brookhaven seem to be more compatible with anomalous transport than the ones from the LHC in Geneva. In Chapter7, a discussion in English and Spanish of the work done and the results obtained in this thesis is included. Finally, a list of all the references cited in the chapters closes the thesis. vii Resumen El transporte anómalo ha despertado gran interés en la última década. Nuevas con- tribuciones no disipativas aparecen en las corrientes de carga y energía como conse- cuencia de la existencia de una anomalía quiral, que es la rotura a nivel cuántico de la simetría quiral. La holografía permite estudiar estos fenómenos de transporte porque se espera que sean importantes en sistemas experimentales en acoplo fuerte. Además, se sabe que la anomalía tiene el mismo valor independientemente de la escala de energías, así que podemos extraer el comportamiento universal del transporte anómalo a través de cálculos en el régimen no perturbativo. Por tanto, en esta tesis usamos la correspondencia AdS/CFT para estudiar diferentes aspectos del transporte in- ducido por anomalías. A continuación resumiremos el contenido de cada capítulo. En el Capítulo1, presentamos el transporte anómalo en relación a los sistemas experimentales en los que aparece y resumimos el contenido del resto de capítu- los. En el Capítulo2, se introduce todo el aparataje teórico necesario para esta tesis. El capítulo posee secciones sobre anomalías, sobre hidrodinámica anómala, sobre teoría de respuesta lineal y sobre holografía. Ambos Capítulos1y2 sirven de intro- ducción. En el Capítulo3, exploramos cómo las simetrías en gravedad pueden ser usadas para simplificar el cálculo de los coeficientes de transporte anómalo. En holografía, la coordenada radial de AdS es dual a una escala de energía de la teoría de cam- pos. Por tanto, los flujos del grupo de renormalización holográfico se pueden en- tender mejor utilizando cargas conservadas radialmente. En trabajos previos se ha mostrado que las simetrías gauge y de difeomorfismos del bulk permiten encontrar cantidades conservadas asociadas a las corrientes de carga y calor.
Recommended publications
  • University of Cincinnati
    UNIVERSITY OF CINCINNATI Date:___________________ I, _________________________________________________________, hereby submit this work as part of the requirements for the degree of: in: It is entitled: This work and its defense approved by: Chair: _______________________________ _______________________________ _______________________________ _______________________________ _______________________________ Topics in supersymmetric gauge theories and the gauge-gravity duality A dissertation submitted to the office of research and advanced studies of the University of Cincinnati in partial fulfillment of the requirements for the degree of Doctor of Philosophy (Ph.D.) in the department of physics of the College of Arts and Sciences B.Sc., Sharif University of Technology, Tehran, Iran, June 2001 Mohammad Edalati Ahmadsaraei June 1, 2007 Dissertation committee chair: Professor Philip C. Argyres Topics in supersymmetric gauge theories and the gauge-gravity duality Mohammad Edalati Ahmadsaraei Department of Physics, University of Cincinnati, P.O. Box 210011, Cincinnati, OH 45221-0011, U.S.A. [email protected] Abstract: In this thesis we use supersymmetry and the gauge-gravity duality to shed light on some dynamical features of strongly-coupled non-Abelian gauge theories. In the first half of the thesis, we consider singular superpotentials of four dimensional = 1 supersymmetric QCD N and show that they must exist. In particular, using some non-trivial consistency checks, we show that these superpotentials, albeit singular, are perfectly sensible, and can be used to reproduce in a simple way both the low energy effective dynamics as well as some special higher-derivative terms. In the second half of the thesis, we investigate the behavior of timelike, spacelike and Euclidean stationary string configurations on a five-dimensional AdS black hole background which, in the context of the gauge-gravity duality, correspond to quark-antiquark pairs steadily moving in an = 4 supersymmetric Yang-Mills thermal N bath.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • Masaki Oshikawa (ISSP, Utokyo) 1 Lecture 1: Anomaly and Condensed Matter Physics
    Symmetry-protected critical phases and global anomaly Croucher Advanced Institute “Topology in Condensed Matter and High-Energy Physics” January 3-5, 2018 @ Chinese University of Hong Kong Masaki Oshikawa (ISSP, UTokyo) 1 Lecture 1: Anomaly and Condensed Matter Physics Lecture II: Symmetry-Protected Critical Phases and Global Anomaly 2 Dirac Fermion massless (m=0) “Dirac cone” 3 Axial Symmetry and Current Massless Dirac fermion Lagrangian density = ¯iγµ@ L µ “vector” U(1) symmetry ⇒ charge current conservation i✓ µ e V @µj =0 ! i✓ µ µ ¯ e− V ¯ j = ¯ ! 2 γµ, γ5 =0 γ5 =1 in even space-time dimensions { } “axial” U(1) symmetry if m=0 ⇒ axial current conservation ei✓A @µj5 =0 ! µ i✓ 5 5 ¯ e A ¯ j = ¯µγ ! µ 4 U(1) Chiral Anomaly Noether’s theorem (“classical”): Massless Dirac fermion ⇒ two conserved currents However, one of these conservation laws is inevitably broken in quantum theory through “regularization” of UV divergence = ¯iγµ(@ iA ) Adler/Bell-Jackiw (1969) L µ − µ Anomalous non-conservation of axial current! µ 5 γ γ 1 @µj5 = ✏ F µ⌫ F ⇢ µ 16⇡2 µ⌫⇢σ Decay of neutral pion ⇡0 γγ (in 3+1 dimensions) 5 ! Regularization/Renormalization “renormalization theory is simply a way to sweep the difficulties of the divergences of electrodynamics under the rug.” Richard Feynman, in Nobel Lecture (1965) 6 Modern Understanding of Renormalization Field theory = universal long-distance behavior of lattice model / condensed matter systems Exact symmetry in the lattice model remains exact in the long-distance limit → no anomaly? Kenneth G. Wilson How can we understand anomaly (1936-2013) in this context? 7 Chiral Anomaly in 1+1 Dim.
    [Show full text]
  • Anomalies in Quantum Field Theory
    Anomalies in Quantum Field Theory Marco Serone SISSA, via Bonomea 265, I-34136 Trieste, Italy Lectures given at the “37th Heidelberg Physics Graduate Days”, 10-14 October 2016 1 Contents 0.1 Introduction.................................... 3 1 Lecture I 5 1.1 Basics of Differential Geometry . 5 1.2 VierbeinsandSpinors ............................. 8 1.3 CharacteristicClasses . 12 2 Lecture II 18 2.1 SupersymmetricQuantumMechanics. .... 18 2.2 AddingGaugeFields............................... 22 2.3 SymmetriesinQFT ............................... 24 2.3.1 WTIdentitiesinQED. 28 3 Lecture III 30 3.1 TheChiralAnomaly ............................... 30 3.2 Consistency Conditions for Gauge and Gravitational Anomalies . 36 4 Lecture IV 39 4.1 The Stora–Zumino Descent Relations . ..... 39 4.2 Path Integral for Gauge and Gravitational Anomalies . ......... 42 4.3 ExplicitformofGaugeAnomaly . 46 5 Lecture V 48 5.1 Chiral and Gauge Anomalies from One-Loop Graphs . ...... 48 5.2 A Relevant Example: Cancellation of Gauge Anomalies in theSM ..... 51 5.3 ’t Hooft Anomaly Matching and the Wess-Zumino-Witten Term ...... 52 5.4 Gravitational Anomalies for Spin 3/2 and Self-Dual Tensors......... 54 2 0.1 Introduction There are different ways of regularizing a Quantum Field Theory (QFT). The best choice of regulator is the one which keeps the maximum number of symmetries of the classical action unbroken. Cut-off regularization, for instance, breaks gauge invariance and that’s why we prefer to work in the somewhat more exotic Dimensional Regularization (DR), where instead gauge invariance is manifestly unbroken. It might happen, however, that there exists no regulator that preserves a given classical symmetry. When this happens, we say that the symmetry is anomalous, namely the quantum theory necessarily breaks it, independently of the choice of regulator.
    [Show full text]
  • Anomalies in Quantum Field Theory
    Anomalies in Quantum Field Theory Marco Serone SISSA, via Bonomea 265, I-34136 Trieste, Italy May 2017 1 Contents 1 Introduction 2 2 Basics of Differential Geometry 3 2.1 VielbeinsandSpinors ............................. 4 2.2 DifferentialForms ................................ 8 2.3 CharacteristicClasses . 11 3 Supersymmetric Quantum Mechanics 17 3.1 AddingGaugeFields............................... 21 4 The Chiral Anomaly 22 5 Consistency Conditions for Gauge and Gravitational Anomalies 28 6 The Stora–Zumino Descent Relations 30 7 Path Integral for Gauge and Gravitational Anomalies 33 7.1 ExplicitformofGaugeAnomaly . 38 8 Gravitational Anomalies for Spin 3/2 and Self-Dual Tensors 40 9 The Green–Schwarz Mechanism 42 10 Non-perturbative Anomalies 45 1 Introduction There are different ways of regularizing a Quantum Field Theory (QFT). The best choice of regulator is the one which keeps the maximum number of symmetries of the classical action unbroken. Cut-off regularization, for instance, breaks gauge invariance while this is unbroken in the somewhat more exotic dimensional regularization. It might happen, how- ever, that there exists no regulator that preserves a given classical symmetry. When this happens, we say that the symmetry is anomalous, namely the quantum theory necessarily breaks it, independently of the choice of regulator. Roughly speaking, anomalies can affect global or local symmetries. The latter case is particularly important, because local symmetries are needed to decouple unphysical states. Indeed, anomalies in linearly realized local gauge symmetries lead to inconsistent theories. Theories with anomalous global symmetries are instead consistent, yet the effect of the 2 anomaly can have important effects. The first anomaly, discovered by Adler, Bell and Jackiw [1], was associated to the non-conservation of the axial current in QCD.
    [Show full text]
  • Global Anomalies on the Hilbert Space
    Global Anomalies on the Hilbert Space Diego Delmastro,ab Davide Gaiotto,a Jaume Gomisa aPerimeter Institute for Theoretical Physics, Waterloo, Ontario, N2L 2Y5, Canada b Department of Physics, University of Waterloo, Waterloo, ON N2L 3G1, Canada Abstract We show that certain global anomalies can be detected in an elementary fashion by analyzing the way the symmetry algebra is realized on the torus Hilbert space of the anomalous theory. Distinct anomalous behaviours imprinted in the Hilbert space are identified with the distinct cohomology \layers" that appear in the classification of anomalies in terms of cobordism groups. We illustrate the manifestation of the layers in the Hilbert for a variety of anomalous symmetries and spacetime dimensions, including time-reversal symmetry, and both in systems of fermions and in anomalous topological quantum field theories (TQFTs) in 2 + 1d. We argue that anomalies can imply an exact bose-fermi degeneracy in the Hilbert space, thus revealing a supersymmetric spectrum of states; we provide a sharp characterization of when this phenomenon occurs and give nontrivial examples in various dimensions, including in strongly coupled QFTs. Unraveling the anomalies of TQFTs leads us to develop the construction of the Hilbert arXiv:2101.02218v2 [hep-th] 18 Aug 2021 spaces, the action of operators and the modular data in spin TQFTs, material that can be read on its own. Contents 1 Introduction and Summary1 2 Anomalies from Layers9 3 Anomalies in free fermion Hilbert space 11 T 3.1 Anomalous Z2 in 0+1 dimensions...................... 11 T 3.2 Anomalous Z4 in 2+1 dimensions...................... 15 3.3 Anomalous Z2 in 1+1 dimensions.....................
    [Show full text]
  • Supersymmetric Tools in Yang-Mills Theories at Strong Coupling: the Beginning of a Long Journey 1 Mikhail Shifman William I
    FTPI-MINN-18/06, UMN-TH-3715/18 Supersymmetric Tools in Yang-Mills Theories at Strong Coupling: the Beginning of a Long Journey 1 Mikhail Shifman William I. Fine Theoretical Physics Institute, University of Minnesota, Minneapolis, MN 55455, USA Abstract Development of holomorphy-based methods in super-Yang-Mills theories started in the early 1980s and lead to a number of breakthrough results. I review some results in which I participated. The discovery of Seiberg's duality and the Seiberg-Witten solution of N = 2 Yang-Mills were the milestones in the long journey of which, I assume, much will be said in other talks. I will focus on the discovery (2003) of non-Abelian vortex strings with various degree of supersymmetry, supported in some four-dimensional Yang-Mills theories and some intriguing implications of this discovery. One of the recent results is the observation of a soliton string in the bulk N = 2 theory with the U(2) gauge group and four flavors, which can become critical in a certain limit. This is the case of a \reverse holography," with a very transparent physical meaning. arXiv:1804.01191v2 [hep-th] 19 Apr 2018 1Based on the talk at the Dirac Medal Award Ceremony, ICTP, March 22, 2017. I should say that receiving the Dirac Medal is the highest honor for me as a the- oretical physicist. I am deeply grateful to Abdus Salam Center for Theoretical Physics for awarding me this highly prestigious Prize. 1 Introduction So far quantum field theory (QFT) remains the basis of our understanding of fun- damental laws of Nature.
    [Show full text]
  • The Standard Model of Particle Physics
    The Standard Model of Particle Physics Uwe-Jens Wiese Institute for Theoretical Physics University of Bern April 11, 2021 Contents 1 Introduction 7 I FUNDAMENTAL CONCEPTS 11 2 Concepts of Quantum Field Theory and the Standard Model 13 2.1 Point Particles versus Fields at the Classical Level . 14 2.2 Particles versus Waves in Quantum Theory . 15 2.3 Classical and Quantum Gauge Fields . 18 2.4 Ultraviolet Divergences, Regularization, and Renormalization 19 2.5 The Standard Model: Renormalizability, Triviality, and Incorporation of Gravity . 20 2.6 Fundamental Standard Model Parameters . 22 2.7 Hierarchies of Scales and Approximate Global Symmetries . 23 2.8 Local and Global Symmetries . 25 2.9 Explicit versus Spontaneous Symmetry Breaking . 27 2.10 Anomalies in Local and Global Symmetries . 28 1 2 CONTENTS 2.11 Euclidean Quantum Field Theory versus Classical Statistical Mechanics . 29 II CONSTRUCTION OF THE STANDARD MODEL 31 3 From Cooper Pairs to Higgs Bosons 33 3.1 A Charged Scalar Field for Cooper Pairs . 34 3.2 The Higgs Doublet . 38 3.3 The Goldstone Theorem . 41 3.4 The Mermin-Wagner Theorem . 44 3.5 Low-Energy Effective Field Theory . 45 3.6 The Hierarchy Problem . 49 3.7 Triviality of the Standard Model . 53 3.8 Electroweak Symmetry Restauration at High Temperature . 55 3.9 Extended Model with Two Higgs Doublets . 56 4 From Superconductivity to Electroweak Gauge Bosons 61 4.1 Scalar Quantum Electrodynamics . 62 4.2 The Higgs Mechanism in the Electroweak Theory . 66 4.3 Accidental Custodial Symmetry . 72 4.4 Lattice Gauge-Higgs Models .
    [Show full text]
  • Anomalies in String Theory with D-Branes*
    ASIAN J. MATH. © 1999 International Press Vol. 3, No. 4, pp. 819-852, December 1999 006 ANOMALIES IN STRING THEORY WITH D-BRANES* DANIEL S. FREEDt AND EDWARD WITTEN* Introduction. This paper is devoted to studying global anomalies in the world- sheet path integral of Type II superstring theory in the presence of D-branes. We will not consider orientifolds (or Type I superstrings) and so our string worldsheets will be oriented Riemann surfaces, mapped to a spacetime manifold Y, which is endowed with a spin structure since the model contains fermions. The first case to consider is that of closed worldsheets, without boundary. In this case, global anomalies cancel, and the worldsheet measure is globally well-defined, given that Y is spin. This is the content of Corollary 4.7 of the present paper; for Y = M10 one has (Theorem 4.8) the further result, related to conformal invariance, that the global anomaly vanishes separately for left- and right-moving degrees of freedom. By contrast, for heterotic strings, global anomaly cancellation gives a restriction that is not evident from the point of view of the low energy effective field theory [W2,F2]. But we will find that Type II global worldsheet anomalies give some novel results when D-branes are present. Thus, we assume the existence of an oriented submanifold Q of spacetime on which strings can end. We then consider a string worldsheet consisting of an oriented surface X that is mapped to Y with <9£ mapped to Q. On Q, there is a field A that is conventionally regarded as a U(l) gauge field, though as we will explain this is not the correct interpretation globally.
    [Show full text]
  • On SU(2) Anomaly and Majorana Fermions
    Article On SU(2) Anomaly and Majorana Fermions Andrei Patrascu Department of Physics and Astronomy, University College London, London WC1E 6BT, UK; [email protected] Academic Editor: Antonio Bianconi Received: 27 January 2017; Accepted: 5 April 2017; Published: 7 April 2017 Abstract: In this paper, a loophole in the SU(2) gauge anomaly is presented. It is shown that using several topological tools, a theory can be designed that implements the quantization of a single Weyl doublet anomaly free while keeping the non-abelian character of the particle in the theory. This opens the perspective for non-Abelian statistics of deconfined particle like objects in 3 + 1 dimensions and for applications in quantum computing. Moreover, if this loophole cannot be closed, old arguments related to anomaly cancellations must be reviewed. Keywords: Witten anomaly; Weyl fermion; Majorana zeromodes; topological phases PACS: 04.20.Cv; 11.15.-q; 04.20.Fy; 03.70.+k 1. Introduction It is a fundamental feature of quantum mechanics that ordinary many particle systems in three dimensions obey one of the two statistics: Bose–Einstein or Fermi–Dirac. Although in most of the textbook applications, this fact is implemented in the form of a postulate, it can also be derived from topological arguments. The main advantage of the topological approach appears in the design of topological quantum computers [1]. Following the ideas of [2], the indiscernibility of particles can be implemented by means of restrictions imposed on the phase space. In fact, the symmetrization (or antisymmetrization) of the standard wavefunction can be traced back to the procedure of identifying the points in the phase space that differ by only a permutation p 2 Sn of the constituent particles.
    [Show full text]
  • Physics Global Gravitational Anomalies
    Communications in Commun. Math. Phys. 100, 197—229 (1985) Mathematical Physics © Springer-Verlag 1985 Global Gravitational Anomalies Edward Witten* Joseph Henry Laboratories, Princeton University, Princeton, NJ 08544, USA Abstract. A general formula for global gauge and gravitational anomalies is derived. It is used to show that the anomaly free supergravity and superstring theories in ten dimensions are all free of global anomalies that might have ruined their consistency. However, it is shown that global anomalies lead to some restrictions on allowed compactifϊcations of these theories. For example, in the case of O(32) superstring theory, it is shown that a global anomaly related to π7(O(32)) leads to a Dirac-like quantization condition for the field strength of the antisymmetric tensor field. Related to global anomalies is the question of the number of fermion zero modes in an instanton field. It is argued that the relevant gravitational instantons are exotic spheres. It is shown that the number of fermion zero modes in an instanton field is always even in ten dimensional supergravity. I. Introduction Anoamlies which arise in perturbation theory [1] can ruin the consistency of quantum field theories. Cancellation of such anomalies is a significant restriction on models in four dimensions [2], and even more so in higher dimensions [3], especially when gravitational and mixed gauge-gravitational anomalies are included [4]. Recently Green and Schwarz have exhibited a new mechanism for anomaly cancellation in higher dimensions [5], which leads to the existence of n = 1 supersymmetric theories with "miraculous" anomaly cancellation in ten dimensions (and O(32) or E8 x E8 gauge group).
    [Show full text]