Conformal Bootstrap in Two-Dimensional Conformal Field Theories with with Non-Diagonal Spectrums Santiago Migliaccio
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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 -
Conformal Bootstrap Signatures of the Tricritical Ising Universality Class
PHYSICAL REVIEW D 101, 116020 (2020) Conformal bootstrap signatures of the tricritical Ising universality class Chethan N. Gowdigere , Jagannath Santara, and Sumedha School of Physical Sciences, National Institute of Science Education and Research, Jatni 752050, India and Homi Bhabha National Institute, Training School Complex, Anushakti Nagar, Mumbai 400094, India (Received 28 November 2018; revised manuscript received 17 April 2020; accepted 12 June 2020; published 30 June 2020) We study the tricritical Ising universality class using conformal bootstrap techniques. By studying bootstrap constraints originating from multiple correlators on the conformal field theory (CFT) data of multiple operator product expansions (OPEs), we are able to determine the scaling dimension of the spin field Δσ in various noninteger dimensions 2 ≤ d ≤ 3. Here, Δσ is connected to the critical exponent η that governs the (tri)critical behavior of the two-point function via the relation η ¼ 2 − d þ 2Δσ. Our results for Δσ match with the exactly known values in two and three dimensions and are a conjecture for noninteger 3 dimensions. We also compare our CFT results for Δσ with ϵ-expansion results, available up to ϵ order. Our techniques can be naturally extended to study higher-order multicritical points. DOI: 10.1103/PhysRevD.101.116020 I. INTRODUCTION the restrictions imposed by conformal invariance and found that the conformal field theory corresponding to The consequences of the conformal hypothesis which the Ising universality class sits on the boundary of the posits conformal invariance to the behavior of physical allowed region at a kinklike point in the space of scaling systems at criticality, in addition to scale invariance, are dimensions of the only two relevant operators. -
Solving the 3D Ising Model with the Conformal Bootstrap Sheer El-Showk, Miguel Paulos, David Poland, Slava Rychkov, David Simmons-Duffin, Alessandro Vichi
Solving the 3D Ising model with the conformal bootstrap Sheer El-Showk, Miguel Paulos, David Poland, Slava Rychkov, David Simmons-Duffin, Alessandro Vichi To cite this version: Sheer El-Showk, Miguel Paulos, David Poland, Slava Rychkov, David Simmons-Duffin, et al.. Solving the 3D Ising model with the conformal bootstrap. Physical Review D, American Physical Society, 2012, 86 (2), pp.25022. 10.1103/PhysRevD.86.025022. cea-00825766 HAL Id: cea-00825766 https://hal-cea.archives-ouvertes.fr/cea-00825766 Submitted on 17 Oct 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. This is the accepted manuscript made available via CHORUS. The article has been published as: Solving the 3D Ising model with the conformal bootstrap Sheer El-Showk, Miguel F. Paulos, David Poland, Slava Rychkov, David Simmons-Duffin, and Alessandro Vichi Phys. Rev. D 86, 025022 — Published 20 July 2012 DOI: 10.1103/PhysRevD.86.025022 LPTENS{12/07 Solving the 3D Ising Model with the Conformal Bootstrap Sheer El-Showka, Miguel F. Paulosb, David Polandc, Slava Rychkovd, David Simmons-Duffine, -
3D Ising Model and Conformal Bootstrap
3D Ising Model and Conformal Bootstrap Slava Rychkov (ENS Paris & CERN) CERN Winter School on Supergravity, Strings, and Gauge Theory 2013 see also “Lectures on CFT in D≥3” @ sites.google.com/site/slavarychkov Part 1 Conformal symmetry (Physical foundations & Basics, Ising model as an example) 2 /60 The subject of these lectures is: The simplest - experimentally relevant - unsolved Conformal Field Theory is 3D Ising Model @ T=Tc It’s also an ideal playground to explain the technique of conformal bootstrap... 3 /60 Basics on the Ising Model cubic lattice → Paradigmatic model of ferromagnetism M- spont. magnetization Tc T Critical temperature (Curie point) 4 /60 Correlation length Critical point can also be detected by looking at the spin-spin correlations For T>Tc : correlation length At T=Tc: Critical theory is scale invariant: It is also conformally invariant [conjectured by Polyakov’71] 5 /60 2D Ising Model • free energy solved by Onsager’44 on the lattice and for any T • Polyakov noticed that is conf. inv. at T=Tc • In 1983 Belavin-Polyakov-Zamolodchikov identified the critical 2D Ising model with the first unitary minimal model 6 /60 3D Ising Model • Lattice model at generic T is probably not solvable [many people tried] • Critical theory (T=Tc) in the continuum limit might be solvable [few people tried, conformal invariance poorly used] 7 /60 Existing approaches to 3D Ising • Lattice Monte-Carlo • High-T expansion on the lattice [~strong coupling expansion] Expand exponential in Converges for T>> Tc , extrapolate for T→ Tc by Pade -
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. -
Pulling Yourself up by Your Bootstraps in Quantum Field Theory
Pulling Yourself Up by Your Bootstraps in Quantum Field Theory Leonardo Rastelli Yang Institute for Theoretical Physics Stony Brook University ICTP and SISSA Trieste, April 3 2019 A. Sommerfeld Center, Munich January 30 2019 Quantum Field Theory in Fundamental Physics Local quantum fields ' (x) f i g x = (t; ~x), with t = time, ~x = space The language of particle physics: for each particle species, a field Quantum Field Theory for Collective Behavior Modelling N degrees of freedom in statistical mechanics. Example: Ising! model 1 (uniaxial ferromagnet) σi = 1, spin at lattice site i ± P Energy H = J σiσj − (ij) Near Tc, field theory description: magnetization '(~x) σ(~x) , ∼ h i Z h i H = d3x ~ ' ~ ' + m2'2 + λ '4 + ::: r · r 2 m T Tc ∼ − Z h i H = d3x ~ ' ~ ' + m2'2 + λ '4 + ::: r · r The dots stand for higher-order \operators": '6, (~ ' ~ ')'2, '8, etc. r · r They are irrelevant for the large-distance physics at T T . ∼ c Crude rule of thumb: an operator is irrelevant if its scaling weight [ ] > 3 (3 d, dimension of space). O O ≡ Basic assignments: ['] = 1 d 1 and [~x] = 1 = [~ ] = 1. 2 ≡ 2 − − ) r So ['2] = 1, ['4] = 2, [~ ' ~ '] =3, while ['8] = 4 etc. r · r First hint of universality: critical exponents do not depend on details. E.g., C T T −α, ' (T T )β for T < T , etc. T ∼ j − cj h i ∼ c − c QFT \Theory of fluctuating fields” (Duh!) ≡ Traditionally, QFT is formulated as a theory of local \quantum fields”: Z H['(x)] Y − Z = d'(x) e g x In particle physics, x spacetime and g = ~ (quantum) 2 In statistical mechanics, x space and g = T (thermal). -
Feynman Diagrams and the Large Charge Expansion in 3−Ε Dimensions
Physics Letters B 802 (2020) 135202 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb Feynman diagrams and the large charge expansion in 3 − ε dimensions ∗ ∗ ∗ ∗ Gil Badel a, , Gabriel Cuomo a, , Alexander Monin a,b, , Riccardo Rattazzi a, a Theoretical Particle Physics Laboratory (LPTP), Institute of Physics, EPFL, Lausanne, Switzerland b Department of Theoretical Physics, University of Geneva, 24 quai Ernest-Ansermet, 1211 Geneva, Switzerland a r t i c l e i n f o a b s t r a c t Article history: In arXiv:1909 .01269 it was shown that the scaling dimension of the lightest charge n operator in the Received 12 December 2019 U (1) model at the Wilson-Fisher fixed point in D = 4 − ε can be computed semiclassically for arbitrary Accepted 6 January 2020 values of λn, where λ is the perturbatively small fixed point coupling. Here we generalize this result to Available online 10 January 2020 the fixed point of the U (1) model in 3 − ε dimensions. The result interpolates continuously between Editor: N. Lambert diagrammatic calculations and the universal conformal superfluid regime for CFTs at large charge. In 0 particular it reproduces the expectedly universal O(n ) contribution to the scaling dimension of large charge operators in 3D CFTs. © 2020 Published by Elsevier B.V. This is an open access article under the CC BY license 3 (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP . 1. Introduction EFT construction, or, in fact, deriving it. This was recently illus- trated in [13], by focusing on the two-point function of the charge n It is known that, even in a weakly coupled Quantum Field n operator φ in the U (1) invariant Wilson-Fisher fixed point in Theory (QFT), there exist situations where the ordinary Feynman 4 − ε dimensions. -
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. -
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. -
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. -
Conformal Bootstrap in Two Dimensions
Conformal Bootstrap in Two Dimensions The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters Citation Lin, Ying-Hsuan. 2016. Conformal Bootstrap in Two Dimensions. Doctoral dissertation, Harvard University, Graduate School of Arts & Sciences. Citable link http://nrs.harvard.edu/urn-3:HUL.InstRepos:33493283 Terms of Use This article was downloaded from Harvard University’s DASH repository, and is made available under the terms and conditions applicable to Other Posted Material, as set forth at http:// nrs.harvard.edu/urn-3:HUL.InstRepos:dash.current.terms-of- use#LAA Conformal Bootstrap in Two Dimensions A dissertation presented by Ying-Hsuan Lin to The Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the subject of Physics Harvard University Cambridge, Massachusetts April 2016 ©2016 - Ying-Hsuan Lin All rights reserved. Thesis advisor Author Xi Yin Ying-Hsuan Lin Conformal Bootstrap in Two Dimensions Abstract In this dissertation, we study bootstrap constraints on conformal field theories in two dimensions. The first half concerns two-dimensional (4; 4) superconformal field theories of cen- tral charge c = 6, corresponding to nonlinear sigma models on K3 surfaces. The superconformal bootstrap is made possible through a surprising relation between the BPS = 4 superconformal blocks with c = 6 and bosonic Virasoro conformal blocks N with c = 28, and an exact moduli dependence of a certain integrated BPS four-point function. Nontrivial bounds on the non-BPS spectrum in the K3 CFT are obtained as functions of the CFT moduli, that interpolate between the free orbifold points and singular CFT points. -
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].