Supersymmetric Field Theories and Isomonodromic Deformations” and the Work Presented in It Are My Own

Total Page:16

File Type:pdf, Size:1020Kb

Supersymmetric Field Theories and Isomonodromic Deformations” and the Work Presented in It Are My Own Scuola Internazionale Superiore di Studi Avanzati - Trieste DOCTORAL THESIS Supersymmetric Field Theories and Isomonodromic Deformations CANDIDATE : Fabrizio Del Monte ADVISORS : Prof. Giulio Bonelli Prof. Alessandro Tanzini OPPONENTS : Dr. Alba Grassi Prof. Andrei Marshakov ACADEMIC YEAR 2019 – 2020 SISSA - Via Bonomea 265 - 34136 TRIESTE - ITALY iii Declaration of Authorship I, Fabrizio DEL MONTE, declare that this thesis titled, “Supersymmetric Field Theories and Isomonodromic Deformations” and the work presented in it are my own. Where I have consulted the published work of others, this is always clearly attributed. The thesis is based on the three research papers • G. Bonelli, F. Del Monte, P. Gavrylenko and A. Tanzini, "N = 2∗ gauge theory, free fermions on the torus and Painlevé VI", Commun. Math. Phys. 377 (2020) no.2, 1381-1419, https://doi.org/10.1007/s00220-020-03743-y; • G. Bonelli, F. Del Monte, P. Gavrylenko and A. Tanzini, "Circular quiver gauge theories, isomonodromic deformations and WN fermions on the torus", https://arxiv.org/abs/1909.07990; • G. Bonelli, F. Del Monte and A. Tanzini, "BPS quivers of five-dimensional SCFTs, Topological Strings and q-Painlevé equations", https://arxiv. org/abs/2007.11596 as well as the still unpublished work • G. Bonelli, F. Del Monte and A. Tanzini, "Higher genus class S theories and isomonodromy", work in progress v SISSA Abstract Doctor of Philosophy Supersymmetric Field Theories and Isomonodromic Deformations by Fabrizio DEL MONTE The topic of this thesis is the recently discovered correspondence between su- persymmetric gauge theories, two-dimensional conformal field theories and isomonodromic deformation problems. Its original results are organized in two parts: the first one, based on the papers [1], [2], as well as on some further unpublished results, provides the extension of the correspondence between four-dimensional class S theories and isomonodromic deformation problems to Riemann Surfaces of genus greater than zero. The second part, based on the results of [3], is instead devoted to the study of five-dimensional super- conformal field theories, and their relation with q-deformed isomonodromic problems. vii Acknowledgements I express my gratitude to my advisors Prof. Giulio Bonelli and Prof. Alessan- dro Tanzini for their important guidance and support, that always helped me to find a direction without ever imposing one. I also thank my collabo- rator and friend Pasha Gavrylenko, with whom I had the fortune of having frequent and prolific discussions that resulted in much of the work in this thesis. I express also my sincerest gratitude to my parents Antonella and Giuseppe that have always supported me and nourished my interests and passions, whether long or short-lived. I want also to thank my past mentors, Kenichi Konishi and Dario Francia: they played a major role in shaping my academic self and my scientific views. I thank all the people that I had the pleasure of discussing during these years, that helped me grow as a person and researcher. Special thanks go to my colleagues and friends at SISSA, that contributed to make sure that my life in Trieste was never boring. I want also to remember all the friends that I left in Lucca, with whom I always look forward to spend time every time I go back. Finally, I thank SISSA and INFN for their continued financial support through all my travels. ix Contents Abstractv Acknowledgements vii I Coulomb Branches and Integrable Systems7 1 Seiberg-Witten Theory and Integrable Systems9 1.1 (Extended) Supersymmetry Algebra in four dimensions....9 1.2 Low-Energy Effective Actions and Prepotentials........ 11 1.3 The Seiberg-Witten Solution.................... 13 1.3.1 Example: Pure Super Yang-Mills............. 14 1.4 Intermezzo: a brief overview of Integrable Systems...... 17 1.5 Seiberg-Witten Theory as an Integrable System......... 20 2 String Theory Embeddings 23 2.1 Witten’s construction of linear quiver theories......... 23 2.2 Class S theories........................... 26 2.3 Intermezzo: Hitchin Systems................... 28 2.4 Hitchin moduli space and Seiberg-Witten theory........ 29 2.5 Geometric Engineering....................... 32 3 Instanton Counting and AGT Correspondence 35 3.1 The instanton moduli space.................... 35 3.2 W-background and instanton partition functions........ 37 3.2.1 Five-dimensional partition functions........... 39 3.3 The AGT correspondence..................... 41 3.3.1 Pants decompositions and conformal blocks...... 44 3.3.2 Topological Vertex, five-dimensional gauge theory and q − WN conformal blocks................. 49 3.4 Surface Operators.......................... 50 3.4.1 M5-brane defects and Kac-Moody Conformal Blocks. 51 3.4.2 M2-brane defects, loop operators and degenerate fields 52 3.5 Fusion, braiding and loop operators............... 53 3.5.1 Fusion algebra of degenerate fields............ 53 3.5.2 Gauge theory loop operators from Verlinde loop oper- ators............................. 57 x II Isomonodromic Deformations and Class S Theories 59 4 Isomonodromic deformations 61 4.1 Painlevé equations......................... 61 4.2 Linear systems of ODEs and isomonodromy.......... 63 4.2.1 Painlevé VI from isomonodromic deformations.... 64 4.3 Isomonodromic deformations and CFT on the Riemann Sphere 66 4.3.1 Free fermion reformulation................ 71 4.4 The Painlevé-Gauge theory correspondence........... 75 5 One-punctured torus, N = 2∗ theory 77 5.1 Isomonodromic deformations and torus conformal blocks.. 77 5.1.1 Linear systems on the torus................ 77 5.1.2 Monodromies of torus conformal blocks......... 80 5.1.3 CFT solution to the Riemann-Hilbert problem and tau function........................... 83 5.2 Tau function and Nekrasov functions.............. 88 5.2.1 Periodicity of the tau functions.............. 88 5.2.2 Asymptotic calculation of the tau function....... 89 Results............................ 90 5.2.3 Asymptotic computation of monodromies....... 92 5.2.4 Initial conditions of Painlevé and Coulomb branch co- ordinates........................... 96 5.2.5 A self-consistency check.................. 96 5.3 Gauge theory, topological strings and Fredholm determinants 99 5.3.1 Line operators and B-branes................ 103 5.3.2 The autonomous/Seiberg-Witten limit.......... 104 6 Torus with many punctures, circular quiver gauge theories 109 6.1 General Fuchsian system on the torus.............. 111 6.2 Kernel and tau function from free fermions........... 113 6.3 Torus monodromies with Verlinde loop operators....... 118 6.3.1 General setup........................ 118 6.3.2 B-cycle monodromy operator............... 120 6.3.3 Fourier transformation................... 122 6.4 Relation to Krichever’s connection................ 124 6.5 Solution of the elliptic Schlesinger system............ 127 7 Higher genus Class S Theories and isomonodromy 131 7.1 Hamiltonian approach to isomonodromic deformations.... 131 7.1.1 Relation to class S theories................. 137 7.1.2 Isomonodromic deformations from flatness of a uni- versal connection...................... 137 7.1.3 Poisson brackets and canonical variables........ 139 7.2 Linear systems and free fermions on Riemann surfaces.... 140 7.3 Conclusions and Outlook..................... 147 xi III Discrete Equations and five-dimensional theories 149 8 Five-dimensional SCFTs and q-Painlevé equations 151 8.1 BPS spectrum of 5d SCFT on S1 and quiver mutations..... 154 8.1.1 Super Yang-Mills, k = 0.................. 155 8.1.2 Super Yang-Mills, k = 1.................. 158 8.1.3 Nf = 2, k = 0........................ 159 8.2 Discrete quiver dynamics, cluster algebras and q-Painlevé.. 165 8.2.1 Cluster algebras and quiver mutations.......... 165 8.2.2 Pure gauge theory and q-Painlevé III3 .......... 168 8.2.3 Super Yang-Mills with two flavors and qPIII1 ...... 171 8.2.4 Super Yang-Mills with two flavours, q-Painlevé IV and q-Painlevé II......................... 174 8.2.5 Summary of dP3 bilinear equations........... 176 8.3 Solutions............................... 176 8.3.1 Local F0 and qPIII3 ..................... 177 8.3.2 q-Painlevé III1 and Nekrasov functions......... 179 8.4 Degeneration of cluster algebras and 4d gauge theory..... 183 8.4.1 From local F0 to the Kronecker quiver.......... 184 8.4.2 Local F1 ........................... 185 8.4.3 Local dP3 .......................... 186 8.5 Conclusions and Outlook..................... 191 IV Appendices 195 A Elliptic and theta functions 197 B Schottky uniformization and twisted differentials 201 C q-Painlevé III and IV in Tsuda’s parametrization 205 C.1 qPIII.................................. 205 C.2 qPIV................................. 206 Bibliography 209 1 Introduction and Summary Quantum Field Theory is the framework allowing to describe physical phe- nomena at all scales, ranging from the astronomical scales of General Rela- tivity, to the everyday physics of conducting metals, all the way to the funda- mental physics at the microscopic level of fundamental particles. In all these applications, however, we can see a common thread: while we can perform approximate computations that are often in spectacular agreement with ex- perimental results, we still have a very poor grasp of the nonperturbative and strongly-coupled aspects of Quantum Field Theory. We can predict to incredible accuracy the anomalous magnetic moment of the electron, but we are still unable to give any quantitative argument for confinement in a real- istic case. A lot of progress, however, has been achieved
Recommended publications
  • Quantum Groups and Algebraic Geometry in Conformal Field Theory
    QUANTUM GROUPS AND ALGEBRAIC GEOMETRY IN CONFORMAL FIELD THEORY DlU'KKERU EI.INKWIJK BV - UTRECHT QUANTUM GROUPS AND ALGEBRAIC GEOMETRY IN CONFORMAL FIELD THEORY QUANTUMGROEPEN EN ALGEBRAISCHE MEETKUNDE IN CONFORME VELDENTHEORIE (mrt em samcnrattint] in hit Stdirlands) PROEFSCHRIFT TER VERKRIJGING VAN DE GRAAD VAN DOCTOR AAN DE RIJKSUNIVERSITEIT TE UTRECHT. OP GEZAG VAN DE RECTOR MAGNIFICUS. TROF. DR. J.A. VAN GINKEI., INGEVOLGE HET BESLUIT VAN HET COLLEGE VAN DE- CANEN IN HET OPENBAAR TE VERDEDIGEN OP DINSDAG 19 SEPTEMBER 1989 DES NAMIDDAGS TE 2.30 UUR DOOR Theodericus Johannes Henrichs Smit GEBOREN OP 8 APRIL 1962 TE DEN HAAG PROMOTORES: PROF. DR. B. DE WIT PROF. DR. M. HAZEWINKEL "-*1 Dit proefschrift kwam tot stand met "•••; financiele hulp van de stichting voor Fundamenteel Onderzoek der Materie (F.O.M.) Aan mijn ouders Aan Saskia Contents Introduction and summary 3 1.1 Conformal invariance and the conformal bootstrap 11 1.1.1 Conformal symmetry and correlation functions 11 1.1.2 The conformal bootstrap program 23 1.2 Axiomatic conformal field theory 31 1.3 The emergence of a Hopf algebra 4G The modular geometry of string theory 56 2.1 The partition function on moduli space 06 2.2 Determinant line bundles 63 2.2.1 Complex line bundles and divisors on a Riemann surface . (i3 2.2.2 Cauchy-Riemann operators (iT 2.2.3 Metrical properties of determinants of Cauchy-Ricmann oper- ators 6!) 2.3 The Mumford form on moduli space 77 2.3.1 The Quillen metric on determinant line bundles 77 2.3.2 The Grothendieck-Riemann-Roch theorem and the Mumford
    [Show full text]
  • Remarks on A2 Toda Field Theory 1 Introduction
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Remarks on A2 Toda Field Theory S. A. Apikyan1 Department of Theoretical Physics Yerevan State University Al. Manoogian 1, Yerevan 375049, Armenia C. Efthimiou2 Department of Physics University of Central Florida Orlando, FL 32816, USA Abstract We study the Toda field theory with finite Lie algebras using an extension of the Goulian-Li technique. In this way, we show that, af- ter integrating over the zero mode in the correlation functions of the exponential fields, the resulting correlation function resembles that of a free theory. Furthermore, it is shown that for some ratios of the charges of the exponential fields the four-point correlation functions which contain a degenerate field satisfy the Riemann ordinary differ- ential equation. Using this fact and the crossing symmetry, we derive a set of functional equations for the structure constants of the A2 Toda field theory. 1 Introduction The Toda field theory (TFT) provides an extremely useful description of a large class of two-dimensional integrable quantum field theories. For this reason these models have attracted a considerable interest in recent years and many outstanding results in various directions have been established. TFTs are divided in three broad categories: finite Toda theories (FTFTs) for which the underlying Kac-Moody algebra [1, 2] is a finite Lie algebra, affine Toda theories (ATFTs) for which the underlying Kac-Moody algebra [email protected] [email protected] 1 is an affine algebra and indefinite Toda theories (ITFTs) for which the under- lying Kac-Moody algebra is an indefinite Kac-Moody algebra.
    [Show full text]
  • An Toda Pmatcd.Pdf
    Kent Academic Repository Full text document (pdf) Citation for published version Adamopoulou, Panagiota and Dunning, Clare (2014) Bethe Ansatz equations for the classical A^(1)_n affine Toda field theories. Journal of Physics A: Mathematical and Theoretical, 47 (20). p. 205205. ISSN 1751-8113. DOI https://doi.org/10.1088/1751-8113/47/20/205205 Link to record in KAR https://kar.kent.ac.uk/40992/ Document Version UNSPECIFIED Copyright & reuse Content in the Kent Academic Repository is made available for research purposes. Unless otherwise stated all content is protected by copyright and in the absence of an open licence (eg Creative Commons), permissions for further reuse of content should be sought from the publisher, author or other copyright holder. Versions of research The version in the Kent Academic Repository may differ from the final published version. Users are advised to check http://kar.kent.ac.uk for the status of the paper. Users should always cite the published version of record. Enquiries For any further enquiries regarding the licence status of this document, please contact: [email protected] If you believe this document infringes copyright then please contact the KAR admin team with the take-down information provided at http://kar.kent.ac.uk/contact.html (1) Bethe Ansatz equations for the classical An affine Toda field theories Panagiota Adamopoulou and Clare Dunning SMSAS, University of Kent, Canterbury, CT2 7NF, United Kingdom E-mails: [email protected], [email protected] Abstract (1) We establish a correspondence between classical An affine Toda field theories and An Bethe Ansatz systems.
    [Show full text]
  • Hamiltonian Reduction and Supersymmetric Toda Models
    UM-P-95/S' QMW-PH-95/7 hep-th/yymmnnn March 1995 Hamiltonian Reduction and Supersymmetric Toda Models G. Au1 and B. Spence2 School of Physics University of Melbourne Parkville 3052 Australia Abstract New formulations of the solutions of N=I and N=2 super Toda field theory are introduced, using Hamiltonian reduction of the N=I and N=2 super WZNW Models to the super Toda Models. These pa- rameterisations are then used to present the HamiJtonian formulations of the super Toda theories on the spaces of solutions. !gauOtauon.ph. unimelb.edu.au [email protected]. Current address: Dept. Physics, Queen Mary & Westfield College, London El 4NS. VQl 2 7 Hi 0 6 1 Introduction Super Toda theories [1, 2, 3, 4, 5] are two dimensional conformal field theories and are an arena for the investigation of general features of two dimensional integrable systems such as quantum supergroups, super W-algebras, and supersymmetric integrable hierachies. The study of many of these properties requires Hamiltonian formulations of the models. The Toda theories can be understood as the Hamiltonian reductions of Wess-Zumino-Novikov-Witten (WZNW) models (see ref. [6]). As the WZNW models are integrable, one can explicitly write a Hamiltonian formulation in terms of the coordinates of the spaces of solutions of the model. In order to preserve full equivalence with the space of initial data, one needs to formulate the WZNW solutions as discussed in ref. [7] (see also ref. [8]). Using this formulation, one may derive, by Hamiltonian reduction, a Hamiltonian formulation of Toda theory [9], utilising suitable coordinates on the space of solutions.
    [Show full text]
  • The Solutions of Affine and Conformal Affine Toda Field Theories
    UM-P-93/75 ' hep-th/9402079 February 1994 The Solutions of Affine and Conformal Affine Toda Field Theories G. PAPADOPOULOS* //. Institute for Theoretical Physics Lumper Chaussee 149 22161 Hamburg Germany and B. SPENCE School of Physics University of Melbourne Parkville 3052 Australia ABSTRACT We give new formulations of the solutions of the field equations of the affine Toda and con- formal afiine Toda theories on a cylinder and two-dimensional Minkowski space-time. These solutions are parameterised in terms of initial data and the resulting covariant phase spaces are diffeomorphic to the Hamiltonian ones. We derive the fundamental Poisson brackets of the parameters of the solutions and give the general static solutions for the affine theory. • E-mail: [email protected] f E-mail: [email protected] 1. Introduction It has been known for many years that the field equations of certain two-dimensional field theories can be solved exactly. Some of these theories are the Wess-Zumino-Witten model, Liouville field theory and and the various versions of Toda field theory. The field equations of these theories are non-linear, partial, hyperbolic differential equations and various dis­ cussions of their solutions have been presented in the literature. One method for solving such integrable systems is based on the theory of Lax pairs and this has been extensively studied for Toda systems [1-3]. These authors solve the field equations on two-dimensional Minkowski space-time and describe their solutions in terms of functions that depend on the light-cone co-ordinates x* of the Minkowski space-time.
    [Show full text]
  • Integrable Deformations of Sine-Liouville Conformal Field Theory and Duality
    Symmetry, Integrability and Geometry: Methods and Applications SIGMA 13 (2017), 080, 22 pages Integrable Deformations of Sine-Liouville Conformal Field Theory and Duality Vladimir A. FATEEV yz y Laboratoire Charles Coulomb UMR 5221 CNRS-UM2, Universit´ede Montpellier, 34095 Montpellier, France E-mail: [email protected] z Landau Institute for Theoretical Physics, 142432 Chernogolovka, Russia Received April 24, 2017, in final form October 03, 2017; Published online October 13, 2017 https://doi.org/10.3842/SIGMA.2017.080 Abstract. We study integrable deformations of sine-Liouville conformal field theory. Eve- ry integrable perturbation of this model is related to the series of quantum integrals of motion (hierarchy). We construct the factorized scattering matrices for different integrable perturbed conformal field theories. The perturbation theory, Bethe ansatz technique, renor- malization group and methods of perturbed conformal field theory are applied to show that all integrable deformations of sine-Liouville model possess non-trivial duality properties. Key words: integrability; duality; Ricci flow 2010 Mathematics Subject Classification: 16T25; 17B68; 83C47 1 Introduction Duality plays an important role in the analysis of statistical, quantum field and string theory systems. Usually it maps a weak coupling region of one theory to the strong coupling region of the other and makes it possible to use perturbative, semiclassical and renormalization group methods in different regions of the coupling constant. For example, the well known duality between sine-Gordon and massive Thirring models [7, 31] together with integrability plays an important role for the justification of exact scattering matrix [39] in these theories. Another well known example of the duality in two-dimensional integrable systems is the weak-strong cou- pling flow from affine Toda theories to the same theories with dual affine Lie algebra [2,6,9].
    [Show full text]
  • Uwaterloo Latex Thesis Template
    The Vertex Algebra Vertex by Miroslav Rapˇc´ak A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree of Doctor of Philosophy in Physics Waterloo, Ontario, Canada, 2019 c Miroslav Rapˇc´ak2019 Examining Committee Membership The following served on the Examining Committee for this thesis. The decision of the Examining Committee is by majority vote. Supervisor: Davide Gaiotto Perimeter Institute for Theoretical Physics Co-supervisor: Jaume Gomis Perimeter Institute for Theoretical Physics Committee Member: Niayesh Afshordi University of Waterloo, Department of Physics and Astronomy Committee Member: Kevin Costello Perimeter Institute for Theoretical Physics Internal/External Member: Benoit Charbonneau University of Waterloo, Department of Pure Mathematics External Examiner: Rajesh Gopakumar International Centre for Theoretical Sciences in Bangalore ii Author's Declaration: I hereby declare that I am the sole author of this thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. iii Abstract This thesis reviews some aspects of a large class of vertex operator algebras labelled by (p; q) webs colored by non-negative integers associated to faces of the web diagrams [1,2,3,4]. Such vertex operator algebras conjecturally correspond to two mutually dual setups in gauge theory. First, they appear as a subsector of local operators living on two- dimensional junctions of half-BPS interfaces in four-dimensional = 4 super Yang-Mills theory. Secondly, they are AGT dual to = 2 gauge theories supportedN on four-cycles inside toric Calabi-Yau three-folds.
    [Show full text]
  • Quantum Solitons in Affine Toda Field Theories
    PUPT-1286 September, 1991 QUANTUM SOLITONS IN AFFINE TODA FIELD THEORIES Timothy Hollowood∗ Joseph Henry Laboratories, Department of Physics, Princeton University, Princeton, N.J. 08544 arXiv:hep-th/9110010v1 3 Oct 1991 ABSTRACT The spectra of Ar affine Toda field theories with imaginary coupling constant, are investi- gated. Soliton solutions are found, which, despite the non-unitary form of the Lagrangian, have real classical masses and are stable to small perturbations. The quantum corrections to the soliton masses are determined, to lowest order in ¯h. The solitons have the same spectrum as the fundamental Toda particles; a feature that is preserved in the quantum theory. ∗ Address after Oct. 1, 1991: Dept. of Theoretical Physics, Oxford, U.K. Introduction Amongst the conformal field theories in two dimensions, there exists a much simpler class of theories, the so-called ‘minimal theories’, whose spectra consist of a finite number of representations of the – possibly extended – conformal algebra [1]. For example, there are the theories where the conformal algebra is extended to the Wr+1-algebras [2]. For each r there exists a whole set of such theories whose central charges are conveniently parameterized in terms of a constant α: 1 2 c = r 1+(r + 1)(r + 2) α + . (1) α ( ) For c r – so α is real – the theories are unitary, but not minimal. For c<r – so α ≥ is purely imaginary – the situation is more complicated: when α2 is rational the theory is minimal, since a finite set of representations decouple from the complete Hilbert space. Furthermore, when α2 takes the particular rational values r + 1 + k α2 = , (2) −r + 2 + k where k is a positive integer, the theory is, in addition, unitary.
    [Show full text]
  • Did a 1-Dimensional Magnet Detect a 248-Dimensional Lie Algebra? David Borthwick, Emory University Skip Garibaldi, Emory University
    Did a 1-dimensional magnet detect a 248-dimensional Lie algebra? David Borthwick, Emory University Skip Garibaldi, Emory University Journal Title: Notices of the American Mathematical Society Volume: Volume 58, Number 8 Publisher: American Mathematical Society | 2011-09, Pages 1055-1066 Type of Work: Article | Final Publisher PDF Permanent URL: http://pid.emory.edu/ark:/25593/d4kgc Final published version: http://www.ams.org/notices/201108/rtx110801055p.pdf Copyright information: © American Mathematical Society Accessed September 28, 2021 9:51 AM EDT Did a 1-Dimensional Magnet Detect a 248-Dimensional Lie Algebra? David Borthwick and Skip Garibaldi ou may have heard some of the buzz symmetry”. No one is claiming to have directly spawned by the recent paper [CTW+] in observed E8. Science. That paper described a neu- Our purpose here is to fill in some of the tron scattering experiment involving details omitted in the previous paragraph. We a quasi-1-dimensional cobalt niobate should explain that we are writing as journalists Y rather than mathematicians here, and we are not magnet and led to rumors that E8 had been de- physicists. We will give pointers to the physics tected “in nature”. This is fascinating, because E8 is a mathematical celebrity and because such a literature so that the adventurous reader can go detection seems impossible: it is hard for us to directly to the words of the experts for complete imagine a realistic experiment that could directly details. observe a 248-dimensional object such as E8. The connection between the cobalt niobate The Ising Model The article in Science describes an experiment experiment and E8 is as follows.
    [Show full text]
  • Renormalization Group Flows and Continual Lie Algebras
    hep–th/0307154 July 2003 Renormalization group flows and continual Lie algebras Ioannis Bakas Department of Physics, University of Patras GR-26500 Patras, Greece [email protected] Abstract We study the renormalization group flows of two-dimensional metrics in sigma models us- ing the one-loop beta functions, and demonstrate that they provide a continual analogue of the Toda field equations in conformally flat coordinates. In this algebraic setting, the logarithm of the world-sheet length scale, t, is interpreted as Dynkin parameter on the root system of a novel continual Lie algebra, denoted by (d/dt; 1), with anti-symmetric G Cartan kernel K(t, t0)=δ0(t t0); as such, it coincides with the Cartan matrix of the − superalgebra sl(N N +1)inthelargeN limit. The resulting Toda field equation is a | non-linear generalization of the heat equation, which is integrable in target space and shares the same dissipative properties in time, t. We provide the general solution of the renormalization group flows in terms of free fields, via B¨acklund transformations, and present some simple examples that illustrate the validity of their formal power series expansion in terms of algebraic data. We study in detail the sausage model that arises as geometric deformation of the O(3) sigma model, and give a new interpretation to its ultra-violet limit by gluing together two copies of Witten’s two-dimensional black hole in the asymptotic region. We also provide some new solutions that describe the renormal- ization group flow of negatively curved spaces in different patches, which look like a cane in the infra-red region.
    [Show full text]
  • Mathematical Physics Studies
    Mathematical Physics Studies Series Editors Giuseppe Dito, Institut de Mathematiques de Bourgogne, Universite de Bourgogne, Dijon, France Edward Frenkel, Department of Mathematics, University of California at Berkley, Berkeley, CA, USA Sergei Gukov, California Institute of Technology, Pasadena, CA, USA Yasuyuki Kawahigashi, Department of Mathematical Sciences, The University of Tokyo, Tokyo, Japan Maxim Kontsevich, Institut des Hautes Etudes Scientifiques, Bures-sur-Yvette, France Nicolaas P. Landsman, Chair of Mathematical Physics, Radboud Universiteit Nijmegen, Nijmegen, Gelderland, The Netherlands Bruno Nachtergaele, Department of Mathematics, University of California, Davis, CA, USA Hal Tasaki, Department of Physics, Gakushuin University, Tokyo, Japan The series publishes original research monographs on contemporary mathematical physics. The focus is on important recent developments at the interface of Mathe- matics, and Mathematical and Theoretical Physics. These will include, but are not restricted to: application of algebraic geometry, D-modules and symplectic geom- etry, category theory, number theory, low-dimensional topology, mirror symmetry, string theory, quantum field theory, noncommutative geometry, operator algebras, functional analysis, spectral theory, and probability theory. More information about this series at http://www.springer.com/series/6316 Taro Kimura Instanton Counting, Quantum Geometry and Algebra Taro Kimura Institut de Mathématiques de Bourgogne Université Bourgogne Franche-Comté Dijon, France ISSN 0921-3767
    [Show full text]
  • Integrable Models and the Toda Lattice Hierarchy
    Integrable Models And The Toda Lattice Hierarchy Bani Mitra Sodermark ∗ Dept of Engineering Sciences, Physics and Mathematics, Karlstad University, 65188 Karlstad, SWEDEN 20 April 1999 Abstract A pedagogical presentation of integrable models with special reference to the Toda lattice hierarchy has been attempted. The example of the KdV equation has been studied in detail, beginning with the infinite conserved quantities and going on to the Lax formalism for the same. We then go on to symplectic manifolds for which we construct the Lax operator. This formalism is applied to Toda Lattice systems. The Zakharov Shabat formalism aimed at encompassing all integrable models is also covered after which the zero curvature condition and its fallout are discussed. We then take up Toda Field Theories and their connection to W algebras via the Hamiltonian reduction of the WZNW model. Finally, we dwell on the connection between four dimensional Yang Mills theories and the KdV equation along with a generalization to supersymmetry. arXiv:hep-th/9906159v1 21 Jun 1999 ∗e.mail: [email protected] 1 1 Introduction: Non-Linear Equations Linear partial differential equations, in particular the Schroedinger, Klein-Gordon and Dirac equations, have been known in field theory over a long time, and have been used in many different problems with great success. Non-linear equations, i.e., equations where the potential term is non-linear in the field (S), have been known for some time as well. These equations and their solutions are the topic of the present Article. The earliest non-linear wave equations known in physics were the Liouville and Sine- Gordon equations.
    [Show full text]