Representation Theory

🧩Representation Theory Unit 1 – Introduction to Group Theory

Group theory explores algebraic structures called groups, focusing on their relationships and symmetries. It provides a framework for understanding mathematical objects and their properties, with applications in physics, chemistry, and computer science. Key concepts include group axioms, subgroups, cosets, and homomorphisms. Various types of groups are studied, such as cyclic, symmetric, and matrix groups. Group theory forms the foundation for representation theory, which examines how abstract groups can be represented as linear transformations.

What's Group Theory All About?

  • Group theory studies algebraic structures called groups which consist of a set of elements and a binary operation that combines any two elements to form a third element in the set
  • Focuses on the relationships and symmetries within these abstract structures rather than the specific nature of the elements themselves
  • Provides a framework for understanding and classifying various mathematical objects and their properties
  • Plays a fundamental role in many branches of mathematics including algebra, geometry, topology, and analysis
  • Has applications beyond pure mathematics in areas such as physics (quantum mechanics, crystallography), chemistry (molecular symmetry), and computer science (cryptography, coding theory)
  • Allows for the development of general theories and techniques that can be applied across different mathematical contexts
  • Enables the identification of common patterns and structures across seemingly disparate mathematical objects

Key Concepts and Definitions

  • A group (G,)(G, *) is a set GG together with a binary operation * that satisfies the following axioms:
    • Closure: For all a,bGa, b \in G, abGa * b \in G
    • Associativity: For all a,b,cGa, b, c \in G, (ab)c=a(bc)(a * b) * c = a * (b * c)
    • Identity element: There exists an element eGe \in G such that for all aGa \in G, ae=ea=aa * e = e * a = a
    • Inverse element: For each aGa \in G, there exists an element a1Ga^{-1} \in G such that aa1=a1a=ea * a^{-1} = a^{-1} * a = e
  • The order of a group G|G| is the number of elements in the set GG
  • A group is called abelian (or commutative) if for all a,bGa, b \in G, ab=baa * b = b * a
  • The center of a group Z(G)Z(G) is the set of elements that commute with every element in the group: Z(G)={aG:ax=xa for all xG}Z(G) = \{a \in G : ax = xa \text{ for all } x \in G\}
  • A subgroup HH of a group GG is a subset of GG that forms a group under the same binary operation as GG
  • The left coset of a subgroup HH in GG with respect to an element aGa \in G is the set aH={ah:hH}aH = \{ah : h \in H\}
  • The right coset of a subgroup HH in GG with respect to an element aGa \in G is the set Ha={ha:hH}Ha = \{ha : h \in H\}

Types of Groups and Examples

  • Cyclic groups: Groups generated by a single element (generator) where every element can be expressed as a power of the generator
    • Example: The group of integers under addition (Z,+)(\mathbb{Z}, +) is cyclic with generator 11 (or 1-1)
    • Example: The group of complex nn-th roots of unity under multiplication is cyclic with generator e2πi/ne^{2\pi i/n}
  • Symmetric groups: Groups of permutations (bijective functions) on a set of nn elements, denoted by SnS_n
    • Example: S3S_3 consists of all permutations of the set {1,2,3}\{1, 2, 3\} under the composition of functions
  • Dihedral groups: Groups of symmetries of regular polygons, including rotations and reflections, denoted by DnD_n for an nn-sided polygon
    • Example: D4D_4 is the group of symmetries of a square, consisting of 4 rotations and 4 reflections
  • Matrix groups: Groups of matrices under matrix multiplication
    • Example: The general linear group GL(n,R)GL(n, \mathbb{R}) consists of all invertible n×nn \times n real matrices
    • Example: The special orthogonal group SO(3)SO(3) consists of all 3×33 \times 3 real orthogonal matrices with determinant 1, representing rotations in 3D space
  • Finite groups: Groups with a finite number of elements
    • Example: The Klein four-group V4V_4 is a finite group of order 4 with elements {e,a,b,c}\{e, a, b, c\} satisfying a2=b2=c2=ea^2 = b^2 = c^2 = e and ab=c,bc=a,ca=bab = c, bc = a, ca = b
  • Infinite groups: Groups with an infinite number of elements
    • Example: The group of real numbers under addition (R,+)(\mathbb{R}, +) is an infinite abelian group

Group Operations and Properties

  • The binary operation of a group can be represented by a group table (Cayley table) which shows the result of combining any two elements
  • A group is called cyclic if it can be generated by a single element, i.e., there exists an element aGa \in G such that every element of GG can be expressed as a power of aa
  • The order of an element aa in a group GG, denoted by a|a|, is the smallest positive integer nn such that an=ea^n = e (if it exists)
    • If no such nn exists, the element is said to have infinite order
  • Lagrange's theorem states that the order of a subgroup divides the order of the group, i.e., if HH is a subgroup of GG, then H|H| divides G|G|
  • The center of a group Z(G)Z(G) is a subgroup of GG and is always abelian
  • A group GG is called simple if it has no proper normal subgroups (subgroups that are invariant under conjugation by elements of GG)
  • The direct product of two groups (G×H,)(G \times H, *) is a group formed by the Cartesian product of the sets GG and HH with the operation defined component-wise: (a,b)(c,d)=(ac,bd)(a, b) * (c, d) = (a*c, b*d)

Subgroups and Cosets

  • A subgroup HH of a group GG must satisfy the following conditions:
    • HH is a non-empty subset of GG
    • For all a,bHa, b \in H, abHa * b \in H (closure under the group operation)
    • For all aHa \in H, a1Ha^{-1} \in H (closure under inverses)
  • The left cosets of a subgroup HH in GG partition the group GG into disjoint sets of equal size
    • The number of left cosets is called the index of HH in GG, denoted by [G:H][G:H]
  • The right cosets of a subgroup HH in GG also partition the group GG into disjoint sets of equal size
  • A subgroup HH is called normal if its left and right cosets coincide, i.e., aH=HaaH = Ha for all aGa \in G
    • Normal subgroups are important because they allow for the construction of quotient groups G/HG/H
  • The kernel of a group homomorphism φ:GG\varphi: G \to G' is a normal subgroup of GG defined as ker(φ)={aG:φ(a)=e}\ker(\varphi) = \{a \in G : \varphi(a) = e'\}, where ee' is the identity element of GG'

Homomorphisms and Isomorphisms

  • A group homomorphism is a function φ:GG\varphi: G \to G' between two groups that preserves the group structure: φ(ab)=φ(a)φ(b)\varphi(a * b) = \varphi(a) *' \varphi(b) for all a,bGa, b \in G, where * and *' are the group operations in GG and GG', respectively
  • The kernel of a homomorphism ker(φ)\ker(\varphi) is always a normal subgroup of the domain group GG
  • The image of a homomorphism Im(φ)={φ(a):aG}\text{Im}(\varphi) = \{\varphi(a) : a \in G\} is a subgroup of the codomain group GG'
  • The first isomorphism theorem states that for a group homomorphism φ:GG\varphi: G \to G', the quotient group G/ker(φ)G/\ker(\varphi) is isomorphic to the image Im(φ)\text{Im}(\varphi)
  • A group isomorphism is a bijective homomorphism, i.e., a one-to-one correspondence between two groups that preserves the group structure
    • Isomorphic groups have the same group-theoretic properties and are essentially the same up to relabeling of elements
  • The automorphism group Aut(G)\text{Aut}(G) of a group GG is the group of all isomorphisms from GG to itself under the composition of functions

Applications in Representation Theory

  • Representation theory studies the ways in which abstract groups can be represented as linear transformations (matrices) acting on vector spaces
  • A representation of a group GG on a vector space VV is a group homomorphism ρ:GGL(V)\rho: G \to GL(V), where GL(V)GL(V) is the general linear group of invertible linear transformations on VV
    • The dimension of the representation is the dimension of the vector space VV
  • The character of a representation ρ\rho is the function χρ:GC\chi_\rho: G \to \mathbb{C} defined by χρ(g)=tr(ρ(g))\chi_\rho(g) = \text{tr}(\rho(g)), where tr\text{tr} denotes the trace of a matrix
    • Characters are class functions, i.e., they are constant on conjugacy classes of GG
  • Irreducible representations are the building blocks of representation theory; they cannot be decomposed into simpler representations
    • Every representation can be written as a direct sum of irreducible representations
  • Schur's lemma states that any linear map between irreducible representations that commutes with the group action is either zero or an isomorphism
  • The regular representation of a finite group GG is the representation on the vector space C[G]\mathbb{C}[G] (the space of complex-valued functions on GG) given by the left regular action of GG on itself
  • Representation theory has applications in physics (symmetries in quantum mechanics), chemistry (molecular symmetry and spectroscopy), and harmonic analysis (Fourier analysis on groups)

Common Pitfalls and Tips

  • Remember that the group operation must be associative; not all binary operations on a set form a group
  • Be careful when dealing with infinite groups; some properties that hold for finite groups may not hold for infinite groups (e.g., not every element has a finite order)
  • When proving that a subset is a subgroup, make sure to check all three conditions (non-empty, closed under the operation, and closed under inverses)
  • Not all subgroups are normal; be cautious when forming quotient groups
  • Lagrange's theorem provides a necessary condition for a subset to be a subgroup, but it is not sufficient (e.g., the alternating group A4A_4 has order 12 but no subgroup of order 6)
  • When working with cosets, remember that they are sets, not elements; use set notation and operations accordingly
  • Homomorphisms and isomorphisms preserve the group structure but not necessarily the properties of individual elements (e.g., the order of an element may change under a homomorphism)
  • In representation theory, the dimension of a representation refers to the dimension of the vector space, not the size of the matrices
  • Characters are a powerful tool in representation theory; they can help determine the irreducibility and equivalence of representations
  • Schur's lemma is a key result in the study of irreducible representations; use it to simplify proofs and computations involving intertwining maps between representations


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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.