Modular Representations of Symmetric Groups
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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 . -
Symmetries on the Lattice
Symmetries On The Lattice K.Demmouche January 8, 2006 Contents Background, character theory of finite groups The cubic group on the lattice Oh Representation of Oh on Wilson loops Double group 2O and spinor Construction of operator on the lattice MOTIVATION Spectrum of non-Abelian lattice gauge theories ? Create gauge invariant spin j states on the lattice Irreducible operators Monte Carlo calculations Extract masses from time slice correlations Character theory of point groups Groups, Axioms A set G = {a, b, c, . } A1 : Multiplication ◦ : G × G → G. A2 : Associativity a, b, c ∈ G ,(a ◦ b) ◦ c = a ◦ (b ◦ c). A3 : Identity e ∈ G , a ◦ e = e ◦ a = a for all a ∈ G. −1 −1 −1 A4 : Inverse, a ∈ G there exists a ∈ G , a ◦ a = a ◦ a = e. Groups with finite number of elements → the order of the group G : nG. The point group C3v The point group C3v (Symmetry group of molecule NH3) c ¡¡AA ¡ A ¡ A Z ¡ A Z¡ A Z O ¡ Z A ¡ Z A ¡ Z A Z ¡ Z A ¡ ZA a¡ ZA b G = {Ra(π),Rb(π),Rc(π),E(2π),R~n(2π/3),R~n(−2π/3)} noted G = {A, B, C, E, D, F } respectively. Structure of Groups Subgroups: Definition A subset H of a group G that is itself a group with the same multiplication operation as G is called a subgroup of G. Example: a subgroup of C3v is the subset E, D, F Classes: Definition An element g0 of a group G is said to be ”conjugate” to another element g of G if there exists an element h of G such that g0 = hgh−1 Example: on can check that B = DCD−1 Conjugacy Class Definition A class of a group G is a set of mutually conjugate elements of G. -
Lie Algebras of Generalized Quaternion Groups 1 Introduction 2
Lie Algebras of Generalized Quaternion Groups Samantha Clapp Advisor: Dr. Brandon Samples Abstract Every finite group has an associated Lie algebra. Its Lie algebra can be viewed as a subspace of the group algebra with certain bracket conditions imposed on the elements. If one calculates the character table for a finite group, the structure of its associated Lie algebra can be described. In this work, we consider the family of generalized quaternion groups and describe its associated Lie algebra structure completely. 1 Introduction The Lie algebra of a group is a useful tool because it is a vector space where linear algebra is available. It is interesting to consider the Lie algebra structure associated to a specific group or family of groups. A Lie algebra is simple if its dimension is at least two and it only has f0g and itself as ideals. Some examples of simple algebras are the classical Lie algebras: sl(n), sp(n) and o(n) as well as the five exceptional finite dimensional simple Lie algebras. A direct sum of simple lie algebras is called a semi-simple Lie algebra. Therefore, it is also interesting to consider if the Lie algebra structure associated with a particular group is simple or semi-simple. In fact, the Lie algebra structure of a finite group is well known and given by a theorem of Cohen and Taylor [1]. In this theorem, they specifically describe the Lie algebra structure using character theory. That is, the associated Lie algebra structure of a finite group can be described if one calculates the character table for the finite group. -
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. -
Representation Theory
M392C NOTES: REPRESENTATION THEORY ARUN DEBRAY MAY 14, 2017 These notes were taken in UT Austin's M392C (Representation Theory) class in Spring 2017, taught by Sam Gunningham. I live-TEXed them using vim, so there may be typos; please send questions, comments, complaints, and corrections to [email protected]. Thanks to Kartik Chitturi, Adrian Clough, Tom Gannon, Nathan Guermond, Sam Gunningham, Jay Hathaway, and Surya Raghavendran for correcting a few errors. Contents 1. Lie groups and smooth actions: 1/18/172 2. Representation theory of compact groups: 1/20/174 3. Operations on representations: 1/23/176 4. Complete reducibility: 1/25/178 5. Some examples: 1/27/17 10 6. Matrix coefficients and characters: 1/30/17 12 7. The Peter-Weyl theorem: 2/1/17 13 8. Character tables: 2/3/17 15 9. The character theory of SU(2): 2/6/17 17 10. Representation theory of Lie groups: 2/8/17 19 11. Lie algebras: 2/10/17 20 12. The adjoint representations: 2/13/17 22 13. Representations of Lie algebras: 2/15/17 24 14. The representation theory of sl2(C): 2/17/17 25 15. Solvable and nilpotent Lie algebras: 2/20/17 27 16. Semisimple Lie algebras: 2/22/17 29 17. Invariant bilinear forms on Lie algebras: 2/24/17 31 18. Classical Lie groups and Lie algebras: 2/27/17 32 19. Roots and root spaces: 3/1/17 34 20. Properties of roots: 3/3/17 36 21. Root systems: 3/6/17 37 22. Dynkin diagrams: 3/8/17 39 23. -
Lecture Notes: Basic Group and Representation Theory
Lecture notes: Basic group and representation theory Thomas Willwacher February 27, 2014 2 Contents 1 Introduction 5 1.1 Definitions . .6 1.2 Actions and the orbit-stabilizer Theorem . .8 1.3 Generators and relations . .9 1.4 Representations . 10 1.5 Basic properties of representations, irreducibility and complete reducibility . 11 1.6 Schur’s Lemmata . 12 2 Finite groups and finite dimensional representations 15 2.1 Character theory . 15 2.2 Algebras . 17 2.3 Existence and classification of irreducible representations . 18 2.4 How to determine the character table – Burnside’s algorithm . 20 2.5 Real and complex representations . 21 2.6 Induction, restriction and characters . 23 2.7 Exercises . 25 3 Representation theory of the symmetric groups 27 3.1 Notations . 27 3.2 Conjugacy classes . 28 3.3 Irreducible representations . 29 3.4 The Frobenius character formula . 31 3.5 The hook lengths formula . 34 3.6 Induction and restriction . 34 3.7 Schur-Weyl duality . 35 4 Lie groups, Lie algebras and their representations 37 4.1 Overview . 37 4.2 General definitions and facts about Lie algebras . 39 4.3 The theorems of Lie and Engel . 40 4.4 The Killing form and Cartan’s criteria . 41 4.5 Classification of complex simple Lie algebras . 43 4.6 Classification of real simple Lie algebras . 44 4.7 Generalities on representations of Lie algebras . 44 4.8 Representation theory of sl(2; C) ................................ 45 4.9 General structure theory of semi-simple Lie algebras . 48 4.10 Representation theory of complex semi-simple Lie algebras . -
Character Theory of Finite Groups NZ Mathematics Research Institute Summer Workshop Day 1: Essentials
1/29 Character Theory of Finite Groups NZ Mathematics Research Institute Summer Workshop Day 1: Essentials Don Taylor The University of Sydney Nelson, 7–13 January 2018 2/29 Origins Suppose that G is a finite group and for every element g G we have 2 an indeterminate xg . What are the factors of the group determinant ¡ ¢ det x 1 ? gh¡ g,h This was a question posed by Dedekind. Frobenius discovered character theory (in 1896) when he set out to answer it. Characters of abelian groups had been used in number theory but Frobenius developed the theory for nonabelian groups. 3/29 Representations Matrices Characters ² ² A linear representation of a group G is a homomorphism ½ : G GL(V ), where GL(V ) is the group of all invertible linear ! transformations of the vector space V , which we assume to have finite dimension over the field C of complex numbers. The dimension n of V is called the degree of ½. If (ei )1 i n is a basis of V , there are functions ai j : G C such that · · ! X ½(x)e j ai j (x)ei . Æ i The matrices A(x) ¡a (x)¢ define a homomorphism A : G GL(n,C) Æ i j ! from G to the group of all invertible n n matrices over C. £ The character of ½ is the function G C that maps x G to Tr(½(x)), ! 2 the trace of ½(x), namely the sum of the diagonal elements of A(x). 4/29 Early applications Frobenius first defined characters as solutions to certain equations. -
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. -
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.