Moonshine Beyond the Monster
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Arxiv:Math/0612474V3 [Math.NT] 23 May 2017 20D08
KAC-MOODY ALGEBRAS, THE MONSTROUS MOONSHINE, JACOBI FORMS AND INFINITE PRODUCTS Jae-Hyun Yang Table of Contents 1. Introduction Notations 2. Kac-Moody Lie Algebras Appendix : Generalized Kac-Moody Algebras 3. The Moonshine Conjectures and the Monster Lie Algebra Appendix : The No-Ghost Theorem 4. Jacobi Forms 5. Infinite Products and Modular Forms 6. Final Remarks 6.1. The Fake Monster Lie Algebras 6.2. Generalized Kac-Moody Algebras of the Arithmetic Type 6.3. Open Problems Appendix A : Classical Modular Forms Appendix B : Kohnen Plus Space and Maass Space arXiv:math/0612474v3 [math.NT] 23 May 2017 Appendix C : The Orthogonal Group Os+2,2(R) Appendix D : The Leech Lattice Λ References This work was in part supported by TGRC-KOSEF. Mathematics Subject Classification (1991) : Primary 11F30, 11F55, 17B65, 17B67, 20C34, 20D08. Typeset by AMS-TEX 1 2 JAE-HYUN YANG 1. Introduction Recently R. E. Borcherds obtained some quite interesting results in [Bo6-7]. First he solved the Moonshine Conjectures made by Conway and Norton([C-N]). Secondly he constructed automorphic forms on the orthogonal group Os+2,2(R) which are modular products and then wrote some of the well-known meromorphic modular forms as infinite products. Modular products roughly mean infinite prod- ucts whose exponents are the coefficients of certain nearly holomorphic modular forms. The theory of Jacobi forms plays an important role in his second work in [Bo7]. More than 10 years ago Feingold and Frenkel([F-F]) realized the connec- tion between the theory of a special hyperbolic Kac-Moody Lie algebra of the type (1) HA1 and that of Jacobi forms of degree one and then generalized the results of H. -
From String Theory and Moonshine to Vertex Algebras
Preample From string theory and Moonshine to vertex algebras Bong H. Lian Department of Mathematics Brandeis University [email protected] Harvard University, May 22, 2020 Dedicated to the memory of John Horton Conway December 26, 1937 – April 11, 2020. Preample Acknowledgements: Speaker’s collaborators on the theory of vertex algebras: Andy Linshaw (Denver University) Bailin Song (University of Science and Technology of China) Gregg Zuckerman (Yale University) For their helpful input to this lecture, special thanks to An Huang (Brandeis University) Tsung-Ju Lee (Harvard CMSA) Andy Linshaw (Denver University) Preample Disclaimers: This lecture includes a brief survey of the period prior to and soon after the creation of the theory of vertex algebras, and makes no claim of completeness – the survey is intended to highlight developments that reflect the speaker’s own views (and biases) about the subject. As a short survey of early history, it will inevitably miss many of the more recent important or even towering results. Egs. geometric Langlands, braided tensor categories, conformal nets, applications to mirror symmetry, deformations of VAs, .... Emphases are placed on the mutually beneficial cross-influences between physics and vertex algebras in their concurrent early developments, and the lecture is aimed for a general audience. Preample Outline 1 Early History 1970s – 90s: two parallel universes 2 A fruitful perspective: vertex algebras as higher commutative algebras 3 Classification: cousins of the Moonshine VOA 4 Speculations The String Theory Universe 1968: Veneziano proposed a model (using the Euler beta function) to explain the ‘st-channel crossing’ symmetry in 4-meson scattering, and the Regge trajectory (an angular momentum vs binding energy plot for the Coulumb potential). -
§2. Elliptic Curves: J-Invariant (Jan 31, Feb 4,7,9,11,14) After
24 JENIA TEVELEV §2. Elliptic curves: j-invariant (Jan 31, Feb 4,7,9,11,14) After the projective line P1, the easiest algebraic curve to understand is an elliptic curve (Riemann surface of genus 1). Let M = isom. classes of elliptic curves . 1 { } We are going to assign to each elliptic curve a number, called its j-invariant and prove that 1 M1 = Aj . 1 1 So as a space M1 A is not very interesting. However, understanding A ! as a moduli space of elliptic curves leads to some breath-taking mathemat- ics. More generally, we introduce M = isom. classes of smooth projective curves of genus g g { } and M = isom. classes of curves C of genus g with points p , . , p C . g,n { 1 n ∈ } We will return to these moduli spaces later in the course. But first let us recall some basic facts about algebraic curves = compact Riemann surfaces. We refer to [G] and [Mi] for a rigorous and detailed exposition. §2.1. Algebraic functions, algebraic curves, and Riemann surfaces. The theory of algebraic curves has roots in analysis of Abelian integrals. An easiest example is the elliptic integral: in 1655 Wallis began to study the arc length of an ellipse (X/a)2 + (Y/b)2 = 1. The equation for the ellipse can be solved for Y : Y = (b/a) (a2 X2), − and this can easily be differentiated !to find bX Y ! = − . a√a2 X2 − 2 This is squared and put into the integral 1 + (Y !) dX for the arc length. Now the substitution x = X/a results in " ! 1 e2x2 s = a − dx, 1 x2 # $ − between the limits 0 and X/a, where e = 1 (b/a)2 is the eccentricity. -
Around Symmetries of Vertex Operator Algebras
Around Symmetries of Vertex Operator Algebras Atsushi Matsuo The University of Tokyo Corrected and revised version of the slides presented for Graphs and Groups, Representations and Relations August 9, 2018 Novosibirsk State University A. Matsuo Around Symmetries of Vertex Operator Algebras 1 x1 Vertex algebras and vertex operator algebras | R.E. Borcherds: Vertex algebras, Kac-Moody algebras and the mon- ster, Proc. Nat. Acad. Sci. U.S.A. 83, (1986), 3068{3071. | I. Frenkel, J. Lepowsky, and A. Meurman: Vertex operator algebras and the Monster, Academic Press, New York, 1988. A. Matsuo Around Symmetries of Vertex Operator Algebras 2 Vertex algebras. A vertex algebra is a vector space V , say over C, equipped with X / −n−1 • A bilinear map V × V V ((z)), (a; b) 7! a(n)bz . n2Z • A nonzero vector 1 2 V , called the vacuum vector. satisfying the following axioms: 2 (1) Borcherds( ) identities. The following holds for all p; q; r Z, X1 p (a b) − c i (r+i) (p+q i) i=0 X1 ( )( ) i r r = (−1) a − (b c) − (−1) b − (a c) : i (p+r i) (q+i) (q+r i) (p+i) i=0 (2) Creation property. { 0; (n ≥ 0), a(n)1 = a; (n = −1). A. Matsuo Around Symmetries of Vertex Operator Algebras 3 Vertex operators. A vertex algebra is specified by the triple (V; Y; 1), where X / −1 −n−1 Y : V (End V )[[z; z ]]; a 7! Y (a; z) = a(n)z : n The generating function Y (a; z) is often called the vertex operator, al- though this term is also used in broader context. -
No. 2, 435-459. Richard E. Borcherds,∗ Mathematics Department, University of California at Berkeley, CA 94720-3840 U
Modular Moonshine II. 24 July 1994, corrected 19 Sept 1995 Duke Math. J. 83 (1996) no. 2, 435-459. Richard E. Borcherds,∗ Mathematics department, University of California at Berkeley, CA 94720-3840 U. S. A. e-mail: [email protected] Alex J. E. Ryba, Dept of Mathematics, Marquette University, Milwaukee, WI 53233, U. S. A. e-mail: [email protected] The monster simple group acts on the monster vertex algebra, and the moonshine conjectures state that the traces of elements of the monster on the vertex algebra are Hauptmoduls. Ryba [R94] conjectured the existence of similar vertex algebras over fields of characteristics p acted on by the centralizers of certain elements of prime order p in the monster, and conjectured that the Brauer traces of p-regular elements of the centralizers were certain Hauptmoduls. We will prove these conjectures when the centralizer involves a sporadic group (p 11, corresponding to the sporadic groups B, F i0 , T h, HN, He, and M12). ≤ 24 Contents. 1. Introduction. Notation. 2. Cohomology and modular representations. 3. Vertex superalgebras mod p. 4. A vanishing theorem for cohomology. 5. The case p = 2. 6. Example: the Held group. 7. Open problems and conjectures. 1. Introduction. The original “moonshine conjectures” of Conway, Norton, McKay, and Thompson said that the monster simple group M has an infinite dimensional graded representation V = n ZVn such that the dimension of Vn n 1 ⊕ ∈ is the coefficient of q of the elliptic modular function j(τ) 744 = q− +196884q+ , and more generally the n − ··· McKay-Thompson series Tg(τ) = n Z Tr(g Vn)q is a Hauptmodul for some genus 0 congruence subgroup P ∈ | of SL2(R). -
Vertex Operator Algebras, the Latter Being a Slightly More Restricted Notion Than the Former (See the Main Text)
Introduction to Vertex Algebras Christophe NOZARADAN† Mathematics department, Universit´eCatholique de Louvain, Louvain-la-Neuve, Belgium e-mail: [email protected] Abstract These lecture notes are intended to give a modest impulse to anyone willing to start or pursue a journey into the theory of vertex algebras by reading one of the books [K1] or [LL]. Therefore, the primary goal is to provide required tools and help being acquainted with the machinery which the whole theory is based on. The exposition follows Kac’s approach [K1]. Fundamental examples relevant in Theoretical Physics are also discussed. No particular prerequisites are assumed. arXiv:0809.1380v3 [math.QA] 11 Nov 2008 Last edited on November 11, 2008. † Research Fellow F.R.S. - FNRS (Aspirant) ii Prologue The notion of vertex algebra1 was first axiomatized by Richard Borcherds in 1986. In retrospect, this algebraic structure has been proved to be equivalent to Conformal Theory of chiral fields in two dimensions [BPZ], for which it provides a rigorous mathematical formulation. Thereby, a new area was born, stressing beautifully the interplay between physics and mathematics. Originally, vertex operators arose in String Theory. They are used to describe certain types of interactions, between different particles or strings, localized at vertices – hence the name“vertex” – of the corresponding Feynman diagrams. From this point of view, the notion of vertex operator thus appeared before the underlying concept of vertex algebra. The concept of vertex algebra happens to be a powerful tool – and initially introduced by Borcherds to this purpose – in the proof [Bo] of the so-called “Moonshine Monstrous” con- jectures, formulated by Conway and Norton. -
Monstrous Moonshine and Monstrous Lie Superalgebras
Monstrous moonshine and monstrous Lie superalgebras. Invent. Math. 109, 405-444 (1992). Richard E. Borcherds, Department of pure mathematics and mathematical statistics, 16 Mill Lane, Cam- bridge CB2 1SB, England. We prove Conway and Norton’s moonshine conjectures for the infinite dimensional representation of the monster simple group constructed by Frenkel, Lepowsky and Meur- man. To do this we use the no-ghost theorem from string theory to construct a family of generalized Kac-Moody superalgebras of rank 2, which are closely related to the monster and several of the other sporadic simple groups. The denominator formulas of these su- peralgebras imply relations between the Thompson functions of elements of the monster (i.e. the traces of elements of the monster on Frenkel, Lepowsky, and Meurman’s repre- sentation), which are the replication formulas conjectured by Conway and Norton. These replication formulas are strong enough to verify that the Thompson functions have most of the “moonshine” properties conjectured by Conway and Norton, and in particular they are modular functions of genus 0. We also construct a second family of Kac-Moody super- algebras related to elements of Conway’s sporadic simple group Co1. These superalgebras have even rank between 2 and 26; for example two of the Lie algebras we get have ranks 26 and 18, and one of the superalgebras has rank 10. The denominator formulas of these algebras give some new infinite product identities, in the same way that the denominator formulas of the affine Kac-Moody algebras give the Macdonald identities. 1 Introduction. 2 Introduction (continued). 3 Vertex algebras. -
A Monster Tale: a Review on Borcherds' Proof of Monstrous Moonshine Conjecture
A monster tale: a review on Borcherds’ proof of monstrous moonshine conjecture by Alan Gerardo Reyes Figueroa Instituto de Matem´atica Pura e Aplicada IMPA A monster tale: a review on Borcherds’ proof of monstrous moonshine conjecture by Alan Gerardo Reyes Figueroa Disserta¸c˜ao Presented in partial fulfillment of the requirements for the degree of Mestre em Matem´atica Instituto de Matem´atica Pura e Aplicada IMPA Maio de 2010 A monster tale: a review on Borcherds’ proof of monstrous moonshine conjecture Alan Gerardo Reyes Figueroa Instituto de Matem´atica Pura e Aplicada APPROVED: 26.05.2010 Hossein Movasati, Ph.D. Henrique Bursztyn, Ph.D. Am´ılcar Pacheco, Ph.D. Fr´ed´eric Paugam, Ph.D. Advisor: Hossein Movasati, Ph.D. v Abstract The Monster M is the largest of the sporadic simple groups. In 1979 Conway and Norton published the remarkable paper ‘Monstrous Moonshine’ [38], proposing a completely unex- pected relationship between finite simple groups and modular functions, in which related the Monster to the theory of modular forms. Conway and Norton conjectured in this paper that there is a close connection between the conjugacy classes of the Monster and the action of certain subgroups of SL2(R) on the upper half plane H. This conjecture implies that extensive information on the representations of the Monster is contained in the classical picture describing the action of SL2(R) on the upper half plane. Monstrous Moonshine is the collection of questions (and few answers) that these observations had directly inspired. In 1988, the book ‘Vertex Operator Algebras and the Monster’ [67] by Frenkel, Lepowsky and Meurman appeared. -
Problems in Moonshine. Richard E. Borcherds, ∗ Mathematics Department, Evans Hall #3840, University of California at Berkeley, CA 94720-3840 U
Problems in moonshine. Richard E. Borcherds, ∗ Mathematics department, Evans Hall #3840, University of California at Berkeley, CA 94720-3840 U. S. A. e-mail: [email protected] www home page www.math.berkeley.edu/˜reb The talk at the I.C.C.M. was an introduction to moonshine. As there are already several survey articles on what is known about moonshine ([B94], [B99], [D-M94], [D- M96], [F-H98], [J]), this paper differs from the talk and will concentrate mainly on what we do not know about it. Moonshine is not a well defined term, but everyone in the area recognizes it when they see it. Roughly speaking, it means weird connections between modular forms and sporadic simple groups. It can also be extended to include related areas such as infinite dimensional Lie algebras or complex hyperbolic reflection groups. Also, it should only be applied to things that are weird and special: if there are an infinite number of examples of something, then it is not moonshine. We first quickly review the original moonshine conjectures of McKay, Thompson, Conway and Norton [C-N]. The classification of finite simple groups shows that every finite simple group either fits into one of about 20 infinite families, or is one of 26 exceptions, called sporadic simple groups. The monster simple group is the largest of the sporadic finite simple groups, and was discovered by Fischer and Griess [G]. Its order is 8080, 17424, 79451, 28758, 86459, 90496, 17107, 57005, 75436, 80000, 00000 =246.320.59.76.112.133.17.19.23.29.31.41.47.59.71 (which is roughly the number of elementary particles in the earth). -
Symmetries, Information and Monster Groups Before and After the Big Bang
information Review Symmetries, Information and Monster Groups before and after the Big Bang Arturo Tozzi 1,* and James F. Peters 2,3 1 Center for Nonlinear Science, University of North Texas, Denton, TX 76203, USA 2 Department of Electrical and Computer Engineering, University of Manitoba, 75A Chancellor’s Circle, Winnipeg, MB R3T 5V6, Canada; [email protected] 3 Mathematics Department, Adıyaman University, 02040 Adıyaman, Turkey * Correspondence: [email protected] Academic Editors: Pedro C. Marijuán, Abir (Andrei) U. Igamberdiev and Lin Bi Received: 5 October 2016; Accepted: 14 December 2016; Published: 21 December 2016 Abstract: The Monster group, the biggest of the sporadic groups, is equipped with the highest known number of dimensions and symmetries. Taking into account variants of the Borsuk–Ulam theorem and a novel topological approach cast in a physical fashion that has the potential to be operationalized, the universe can be conceived as a lower-dimensional manifold encompassed in the Monster group. Our universe might arise from spontaneous dimension decrease and symmetry breaking that occur inside the very structure of the Monster Module. We elucidate how the energetic loss caused by projection from higher to lower dimensions and by the Monster group’s non-abelian features is correlated with the present-day asymmetry in the thermodynamic arrow. By linking the Monster Module to its theoretical physical counterparts, it is then possible to calculate its enthalpy and Lie group trajectories. Our approach also reveals how a symmetry break might lead to a universe based on multi-dimensional string theories and CFT/AdS (anti-de Sitter/conformal field theory) correspondence. -
Arxiv:0910.3145V1 [Hep-Th] 16 Oct 2009 Fphysics: of Navneoraooist Vroewoewr a Eninap Been Has Work Kno Whose Limited Everyone the to to and Omitted
ZMP-HH/09-21 Hamburger Beitr¨age zur Mathematik Nr. 349 October 2009 TWENTY-FIVE YEARS OF TWO-DIMENSIONAL RATIONAL CONFORMAL FIELD THEORY J¨urgen Fuchs a, Ingo Runkel b and Christoph Schweigert b a Teoretisk fysik, Karlstads Universitet Universitetsgatan 21, S–65188 Karlstad b Organisationseinheit Mathematik, Universit¨at Hamburg Bereich Algebra und Zahlentheorie Bundesstraße 55, D–20146 Hamburg A review for the 50th anniversary of the Journal of Mathematical Physics. 1 Introduction In this article we try to give a condensed panoramic view of the development of two-dimen- sional rational conformal field theory in the last twenty-five years. Given its limited length, our contribution can be, at best, a collection of pointers to the literature. Needless to say, the arXiv:0910.3145v1 [hep-th] 16 Oct 2009 exposition is highly biased, by the taste and the limited knowledge of the authors. We present in advance our apologies to everyone whose work has been inappropriately represented or even omitted. The study of conformal field theories in two dimensions has its origin in several distinct areas of physics: • In the attempt to describe the strong interactions in elementary particle physics in the frame- work of dual models. • Under the label string theory, these models were reinterpreted as a perturbation series containing a gravitational sector. Conformal field theories appear as theories defined on the world sheet that is swept out by the string [56]. • In statistical mechanics, conformal field theory plays a fundamental role in the theory of two- dimensional critical systems [189, 92] by describing fixed points of the renormalization group. -
Vertex Algebra Constructions of Generalized Kac-Moody Algebras — an Overview
Vertex Algebra constructions of Generalized Kac-Moody Algebras — An overview Gerald H¨ohn Kansas State University September 1, 2009 Definition A vertex operator algebra (VOA) of central charge c consists of L∞ I a Z+-graded complex vector space V = m=0 Vm (state space) with dim Vm < ∞ and dim V0 = 1; I a vector 1 ∈ V0 (vacuum vector); I a linear map Y ( ., z): V −→ End(V )[[z, z−1]] (vertex operator) P −n−1 which maps a ∈ Vm to Y (a, z) = z such that an n∈Z has degree −n − 1 + m and for all v ∈ V one has anv = 0 for large enough n. I a vector ω ∈ V2 (Virasoro vector); such that the following axioms are satisfied: Definition A vertex operator algebra (VOA) of central charge c consists of a tuple (V , 1Y , ω) such that the following axioms are satisfied: I Y (1, z) = idV , and for all a ∈ V one has Y (a, z)1 ∈ V [[z]] with Y (a, z)1|z=0 = a (vacuum axiom); I For all a, b ∈ V there exists an N ∈ Z+ such that (z − w)N Y (a, z)Y (b, w) = (z − w)N Y (b, w) (locality axiom); P −n−2 for Y (ω, z) = Lnz one has (Virasoro axioms) I n∈Z I L0|Vm = m · id|Vm , I L−11 = 0 and [L−1, Y (a, z)] = ∂z Y (a, z) for all a ∈ V , c I L2ω = 2 · 1. Remark P −n−2 The coefficients of Y (ω, z) = Lnz satisfy the n∈Z commutator relations of the Virasoro algebra: n3 − n [L , L ] = (n − m)L + δ · c · id .