Some Moonshine Connections Between Fischer-Griess Monster Group () and Number Theory
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NOTES on FINITE GROUP REPRESENTATIONS in Fall 2020, I
NOTES ON FINITE GROUP REPRESENTATIONS CHARLES REZK In Fall 2020, I taught an undergraduate course on abstract algebra. I chose to spend two weeks on the theory of complex representations of finite groups. I covered the basic concepts, leading to the classification of representations by characters. I also briefly addressed a few more advanced topics, notably induced representations and Frobenius divisibility. I'm making the lectures and these associated notes for this material publicly available. The material here is standard, and is mainly based on Steinberg, Representation theory of finite groups, Ch 2-4, whose notation I will mostly follow. I also used Serre, Linear representations of finite groups, Ch 1-3.1 1. Group representations Given a vector space V over a field F , we write GL(V ) for the group of bijective linear maps T : V ! V . n n When V = F we can write GLn(F ) = GL(F ), and identify the group with the group of invertible n × n matrices. A representation of a group G is a homomorphism of groups φ: G ! GL(V ) for some representation choice of vector space V . I'll usually write φg 2 GL(V ) for the value of φ on g 2 G. n When V = F , so we have a homomorphism φ: G ! GLn(F ), we call it a matrix representation. matrix representation The choice of field F matters. For now, we will look exclusively at the case of F = C, i.e., representations in complex vector spaces. Remark. Since R ⊆ C is a subfield, GLn(R) is a subgroup of GLn(C). -
Molecular Symmetry
Molecular Symmetry Symmetry helps us understand molecular structure, some chemical properties, and characteristics of physical properties (spectroscopy) – used with group theory to predict vibrational spectra for the identification of molecular shape, and as a tool for understanding electronic structure and bonding. Symmetrical : implies the species possesses a number of indistinguishable configurations. 1 Group Theory : mathematical treatment of symmetry. symmetry operation – an operation performed on an object which leaves it in a configuration that is indistinguishable from, and superimposable on, the original configuration. symmetry elements – the points, lines, or planes to which a symmetry operation is carried out. Element Operation Symbol Identity Identity E Symmetry plane Reflection in the plane σ Inversion center Inversion of a point x,y,z to -x,-y,-z i Proper axis Rotation by (360/n)° Cn 1. Rotation by (360/n)° Improper axis S 2. Reflection in plane perpendicular to rotation axis n Proper axes of rotation (C n) Rotation with respect to a line (axis of rotation). •Cn is a rotation of (360/n)°. •C2 = 180° rotation, C 3 = 120° rotation, C 4 = 90° rotation, C 5 = 72° rotation, C 6 = 60° rotation… •Each rotation brings you to an indistinguishable state from the original. However, rotation by 90° about the same axis does not give back the identical molecule. XeF 4 is square planar. Therefore H 2O does NOT possess It has four different C 2 axes. a C 4 symmetry axis. A C 4 axis out of the page is called the principle axis because it has the largest n . By convention, the principle axis is in the z-direction 2 3 Reflection through a planes of symmetry (mirror plane) If reflection of all parts of a molecule through a plane produced an indistinguishable configuration, the symmetry element is called a mirror plane or plane of symmetry . -
Arxiv:1911.10534V3 [Math.AT] 17 Apr 2020 Statement
THE ANDO-HOPKINS-REZK ORIENTATION IS SURJECTIVE SANATH DEVALAPURKAR Abstract. We show that the map π∗MString ! π∗tmf induced by the Ando-Hopkins-Rezk orientation is surjective. This proves an unpublished claim of Hopkins and Mahowald. We do so by constructing an E1-ring B and a map B ! MString such that the composite B ! MString ! tmf is surjective on homotopy. Applications to differential topology, and in particular to Hirzebruch's prize question, are discussed. 1. Introduction The goal of this paper is to show the following result. Theorem 1.1. The map π∗MString ! π∗tmf induced by the Ando-Hopkins-Rezk orientation is surjective. This integral result was originally stated as [Hop02, Theorem 6.25], but, to the best of our knowledge, no proof has appeared in the literature. In [HM02], Hopkins and Mahowald give a proof sketch of Theorem 1.1 for elements of π∗tmf of Adams-Novikov filtration 0. The analogue of Theorem 1.1 for bo (namely, the statement that the map π∗MSpin ! π∗bo induced by the Atiyah-Bott-Shapiro orientation is surjective) is classical [Mil63]. In Section2, we present (as a warmup) a proof of this surjectivity result for bo via a technique which generalizes to prove Theorem 1.1. We construct an E1-ring A with an E1-map A ! MSpin. The E1-ring A is a particular E1-Thom spectrum whose mod 2 homology is given by the polynomial subalgebra 4 F2[ζ1 ] of the mod 2 dual Steenrod algebra. The Atiyah-Bott-Shapiro orientation MSpin ! bo is an E1-map, and so the composite A ! MSpin ! bo is an E1-map. -
GROUP REPRESENTATIONS and CHARACTER THEORY Contents 1
GROUP REPRESENTATIONS AND CHARACTER THEORY DAVID KANG Abstract. In this paper, we provide an introduction to the representation theory of finite groups. We begin by defining representations, G-linear maps, and other essential concepts before moving quickly towards initial results on irreducibility and Schur's Lemma. We then consider characters, class func- tions, and show that the character of a representation uniquely determines it up to isomorphism. Orthogonality relations are introduced shortly afterwards. Finally, we construct the character tables for a few familiar groups. Contents 1. Introduction 1 2. Preliminaries 1 3. Group Representations 2 4. Maschke's Theorem and Complete Reducibility 4 5. Schur's Lemma and Decomposition 5 6. Character Theory 7 7. Character Tables for S4 and Z3 12 Acknowledgments 13 References 14 1. Introduction The primary motivation for the study of group representations is to simplify the study of groups. Representation theory offers a powerful approach to the study of groups because it reduces many group theoretic problems to basic linear algebra calculations. To this end, we assume that the reader is already quite familiar with linear algebra and has had some exposure to group theory. With this said, we begin with a preliminary section on group theory. 2. Preliminaries Definition 2.1. A group is a set G with a binary operation satisfying (1) 8 g; h; i 2 G; (gh)i = g(hi)(associativity) (2) 9 1 2 G such that 1g = g1 = g; 8g 2 G (identity) (3) 8 g 2 G; 9 g−1 such that gg−1 = g−1g = 1 (inverses) Definition 2.2. -
Our Mathematical Universe: I. How the Monster Group Dictates All of Physics
October, 2011 PROGRESS IN PHYSICS Volume 4 Our Mathematical Universe: I. How the Monster Group Dictates All of Physics Franklin Potter Sciencegems.com, 8642 Marvale Drive, Huntington Beach, CA 92646. E-mail: [email protected] A 4th family b’ quark would confirm that our physical Universe is mathematical and is discrete at the Planck scale. I explain how the Fischer-Greiss Monster Group dic- tates the Standard Model of leptons and quarks in discrete 4-D internal symmetry space and, combined with discrete 4-D spacetime, uniquely produces the finite group Weyl E8 x Weyl E8 = “Weyl” SO(9,1). The Monster’s j-invariant function determines mass ratios of the particles in finite binary rotational subgroups of the Standard Model gauge group, dictates Mobius¨ transformations that lead to the conservation laws, and connects interactions to triality, the Leech lattice, and Golay-24 information coding. 1 Introduction 5. Both 4-D spacetime and 4-D internal symmetry space are discrete at the Planck scale, and both spaces can The ultimate idea that our physical Universe is mathematical be telescoped upwards mathematically by icosians to at the fundamental scale has been conjectured for many cen- 8-D spaces that uniquely combine into 10-D discrete turies. In the past, our marginal understanding of the origin spacetime with discrete Weyl E x Weyl E symmetry of the physical rules of the Universe has been peppered with 8 8 (not the E x E Lie group of superstrings/M-theory). huge gaps, but today our increased understanding of funda- 8 8 mental particles promises to eliminate most of those gaps to 6. -
§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. -
Representations, Character Tables, and One Application of Symmetry Chapter 4
Representations, Character Tables, and One Application of Symmetry Chapter 4 Friday, October 2, 2015 Matrices and Matrix Multiplication A matrix is an array of numbers, Aij column columns matrix row matrix -1 4 3 1 1234 rows -8 -1 7 2 2141 3 To multiply two matrices, add the products, element by element, of each row of the first matrix with each column in the second matrix: 12 12 (1×1)+(2×3) (1×2)+(2×4) 710 × 34 34 = (3×1)+(4×3) (3×2)+(4×4) = 15 22 100 1 1 0-10× 2 = -2 002 3 6 Transformation Matrices Each symmetry operation can be represented by a 3×3 matrix that shows how the operation transforms a set of x, y, and z coordinates y Let’s consider C2h {E, C2, i, σh}: x transformation matrix C2 x’ = -x -1 0 0 x’ -1 0 0 x -x y’ = -y 0-10 y’ ==0-10 y -y z’ = z 001 z’ 001 z z new transformation old new in terms coordinates ==matrix coordinates of old transformation i matrix x’ = -x -1 0 0 x’ -1 0 0 x -x y’ = -y 0-10 y’ ==0-10 y -y z’ = -z 00-1 z’ 00-1z -z Representations of Groups The set of four transformation matrices forms a matrix representation of the C2h point group. 100 -1 0 0 -1 0 0 100 E: 010 C2: 0-10 i: 0-10 σh: 010 001 001 00-1 00-1 These matrices combine in the same way as the operations, e.g., -1 0 0 -1 0 0 100 C2 × C2 = 0-10 0-10= 010= E 001001 001 The sum of the numbers along each matrix diagonal (the character) gives a shorthand version of the matrix representation, called Γ: C2h EC2 i σh Γ 3-1-31 Γ (gamma) is a reducible representation b/c it can be further simplified. -
K3 Surfaces, N= 4 Dyons, and the Mathieu Group
K3 Surfaces, =4 Dyons, N and the Mathieu Group M24 Miranda C. N. Cheng Department of Physics, Harvard University, Cambridge, MA 02138, USA Abstract A close relationship between K3 surfaces and the Mathieu groups has been established in the last century. Furthermore, it has been observed recently that the elliptic genus of K3 has a natural inter- pretation in terms of the dimensions of representations of the largest Mathieu group M24. In this paper we first give further evidence for this possibility by studying the elliptic genus of K3 surfaces twisted by some simple symplectic automorphisms. These partition functions with insertions of elements of M24 (the McKay-Thompson series) give further information about the relevant representation. We then point out that this new “moonshine” for the largest Mathieu group is con- nected to an earlier observation on a moonshine of M24 through the 1/4-BPS spectrum of K3 T 2-compactified type II string theory. This insight on the symmetry× of the theory sheds new light on the gener- alised Kac-Moody algebra structure appearing in the spectrum, and leads to predictions for new elliptic genera of K3, perturbative spec- arXiv:1005.5415v2 [hep-th] 3 Jun 2010 trum of the toroidally compactified heterotic string, and the index for the 1/4-BPS dyons in the d = 4, = 4 string theory, twisted by elements of the group of stringy K3N isometries. 1 1 Introduction and Summary Recently there have been two new observations relating K3 surfaces and the largest Mathieu group M24. They seem to suggest that the sporadic group M24 naturally acts on the spectrum of K3-compactified string theory. -
Lecture Notes
i Applications of Group Theory to the Physics of Solids M. S. Dresselhaus 8.510J 6.734J SPRING 2002 ii Contents 1 Basic Mathematical Background 1 1.1 De¯nition of a Group . 1 1.2 Simple Example of a Group . 2 1.3 Basic De¯nitions . 4 1.4 Rearrangement Theorem . 6 1.5 Cosets . 6 1.6 Conjugation and Class . 8 1.6.1 Self-Conjugate Subgroups . 9 1.7 Factor Groups . 10 1.8 Selected Problems . 11 2 Representation Theory 15 2.1 Important De¯nitions . 15 2.2 Matrices . 17 2.3 Irreducible Representations . 18 2.4 The Unitarity of Representations . 20 2.5 Schur's Lemma (Part I) . 23 2.6 Schur's Lemma (Part 2) . 24 2.7 Wonderful Orthogonality Theorem . 27 2.8 Representations and Vector Spaces . 30 2.9 Suggested Problems . 31 3 Character of a Representation 33 3.1 De¯nition of Character . 33 3.2 Characters and Class . 34 3.3 Wonderful Orthogonality Theorem for Character . 36 3.4 Reducible Representations . 38 iii iv CONTENTS 3.5 The Number of Irreducible Representations . 40 3.6 Second Orthogonality Relation for Characters . 41 3.7 Regular Representation . 43 3.8 Setting up Character Tables . 47 3.9 Symmetry Notation . 51 3.10 Selected Problems . 73 4 Basis Functions 75 4.1 Symmetry Operations and Basis Functions . 75 4.2 Basis Functions for Irreducible Representations . 77 ^(¡n) 4.3 Projection Operators Pkl . 82 ^(¡n) 4.4 Derivation of Pk` . 83 4.5 Projection Operations on an Arbitrary Function . 84 4.6 Linear Combinations for 3 Equivalent Atoms . -
The Q-Conjugacy Character Table of Dihedral Groups
ITALIAN JOURNAL OF PURE AND APPLIED MATHEMATICS { N. 39{2018 (89{96) 89 THE Q-CONJUGACY CHARACTER TABLE OF DIHEDRAL GROUPS H. Shabani A. R. Ashrafi E. Haghi Department of Pure Mathematics Faculty of Mathematical Sciences University of Kashan P.O. Box 87317-53153 Kashan I.R. Iran M. Ghorbani∗ Department of Pure Mathematics Faculty of Sciences Shahid Rajaee Teacher Training University P.O. Box 16785-136 Tehran I.R. Iran [email protected] Abstract. In a seminal paper published in 1998, Shinsaku Fujita introduced the concept of Q-conjugacy character table of a finite group. He applied this notion to solve some problems in combinatorial chemistry. In this paper, the Q-conjugacy character table of dihedral groups is computed in general. As a consequence, Q- ∼ ∼ conjugacy character table of molecules with point group symmetries D = C = Dih , ∼ ∼ ∼ ∼ ∼ ∼ ∼ ∼3 3v∼ 6 D = D = C = Dih , D = C = Dih , D = D = D = C = Dih , 4 ∼ 2d ∼ 4v ∼ 8 5 ∼5v 10 ∼3d ∼3h 6 ∼6v 12 D2 = C2v = Z2 × Z2 = Dih2, D4d = Dih16, D5d = D5h = Dih20, D6d = Dih24 are computed, where Z2 denotes a cyclic group of order 2 and Dihn is the dihedral group of even order n. Keywords: Q-conjugacy character table, dihedral group, conjugacy class. 1. Introduction A representation of a group G is a homomorphism from G into the group of invertible operators of a vector space V . In this case, we can interpret each element of G as an invertible linear transformation V −! V . If n = dimV and fix a basis for V then we can construct an isomorphism between the set of all \invertible linear transformation V −! V " and the set of all \invertible n × n matrices". -
Irreducible Representations and Character Tables
MIT OpenCourseWare http://ocw.mit.edu 5.04 Principles of Inorganic Chemistry II �� Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 5.04, Principles of Inorganic Chemistry II Prof. Daniel G. Nocera Lecture 3: Irreducible Representations and Character Tables Similarity transformations yield irreducible representations, Γi, which lead to the useful tool in group theory – the character table. The general strategy for determining Γi is as follows: A, B and C are matrix representations of symmetry operations of an arbitrary basis set (i.e., elements on which symmetry operations are performed). There is some similarity transform operator v such that A’ = v –1 ⋅ A ⋅ v B’ = v –1 ⋅ B ⋅ v C’ = v –1 ⋅ C ⋅ v where v uniquely produces block-diagonalized matrices, which are matrices possessing square arrays along the diagonal and zeros outside the blocks ⎡ A1 ⎤ ⎡B1 ⎤ ⎡C1 ⎤ ′ = ⎢ ⎥ ′ = ⎢ ⎥ ′ = ⎢ ⎥ A ⎢ A 2 ⎥ B ⎢ B2 ⎥ C ⎢ C 2 ⎥ ⎢ A ⎥ ⎢ B ⎥ ⎢ C ⎥ ⎣ 3 ⎦ ⎣ 3 ⎦ ⎣ 3 ⎦ Matrices A, B, and C are reducible. Sub-matrices Ai, Bi and Ci obey the same multiplication properties as A, B and C. If application of the similarity transform does not further block-diagonalize A’, B’ and C’, then the blocks are irreducible representations. The character is the sum of the diagonal elements of Γi. 2 As an example, let’s continue with our exemplary group: E, C3, C3 , σv, σv’, σv” by defining an arbitrary basis … a triangle v A v'' v' C B The basis set is described by the triangles vertices, points A, B and C. -
Moonshines for L2(11) and M12
Moonshines for L2(11) and M12 Suresh Govindarajan Department of Physics Indian Institute of Technology Madras (Work done with my student Sutapa Samanta) Talk at the Workshop on Modular Forms and Black Holes @NISER, Bhubaneswar on January 13. 2017 Plan Introduction Some finite group theory Moonshine BKM Lie superalgebras Introduction Classification of Finite Simple Groups Every finite simple group is isomorphic to one of the following groups: (Source: Wikipedia) I A cyclic group with prime order; I An alternating group of degree at least 5; I A simple group of Lie type, including both I the classical Lie groups, namely the groups of projective special linear, unitary, symplectic, or orthogonal transformations over a finite field; I the exceptional and twisted groups of Lie type (including the Tits group which is not strictly a group of Lie type). I The 26 sporadic simple groups. The classification was completed in 2004 when Aschbacher and Smith filled the last gap (`the quasi-thin case') in the proof. Fun Reading: Symmetry and the Monster by Mark Ronan The sporadic simple groups I the Mathieu groups: M11, M12, M22, M23, M24; (found in 1861) I the Janko groups: J1, J2, J3, J4; (others 1965-1980) I the Conway groups; Co1, Co2, Co3; 0 I the Fischer groups; Fi22. Fi23, Fi24; I the Higman-Sims group; HS I the McLaughlin group: McL I the Held group: He; I the Rudvalis group Ru; I the Suzuki sporadic group: Suz; 0 I the O'Nan group: O N; I Harada-Norton group: HN; I the Lyons group: Ly; I the Thompson group: Th; I the baby Monster group: B and Sources: Wikipedia and Mark Ronan I the Fischer-Griess Monster group: M Monstrous Moonshine Conjectures I The j-function has the followed q-series: (q = exp(2πiτ)) j(τ)−744 = q−1+[196883+1] q+[21296876+196883+1] q2+··· I McKay observed that 196883 and 21296876 are the dimensions of the two smallest irreps of the Monster group.