🧩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.
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,∗) is a set G together with a binary operation ∗ that satisfies the following axioms:
Closure: For all a,b∈G, a∗b∈G
Associativity: For all a,b,c∈G, (a∗b)∗c=a∗(b∗c)
Identity element: There exists an element e∈G such that for all a∈G, a∗e=e∗a=a
Inverse element: For each a∈G, there exists an element a−1∈G such that a∗a−1=a−1∗a=e
The order of a group ∣G∣ is the number of elements in the set G
A group is called abelian (or commutative) if for all a,b∈G, a∗b=b∗a
The center of a group Z(G) is the set of elements that commute with every element in the group: Z(G)={a∈G:ax=xa for all x∈G}
A subgroup H of a group G is a subset of G that forms a group under the same binary operation as G
The left coset of a subgroup H in G with respect to an element a∈G is the set aH={ah:h∈H}
The right coset of a subgroup H in G with respect to an element a∈G is the set Ha={ha:h∈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,+) is cyclic with generator 1 (or −1)
Example: The group of complex n-th roots of unity under multiplication is cyclic with generator e2πi/n
Symmetric groups: Groups of permutations (bijective functions) on a set of n elements, denoted by Sn
Example: S3 consists of all permutations of the set {1,2,3} under the composition of functions
Dihedral groups: Groups of symmetries of regular polygons, including rotations and reflections, denoted by Dn for an n-sided polygon
Example: D4 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) consists of all invertible n×n real matrices
Example: The special orthogonal group SO(3) consists of all 3×3 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 V4 is a finite group of order 4 with elements {e,a,b,c} satisfying a2=b2=c2=e and ab=c,bc=a,ca=b
Infinite groups: Groups with an infinite number of elements
Example: The group of real numbers under addition (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 a∈G such that every element of G can be expressed as a power of a
The order of an element a in a group G, denoted by ∣a∣, is the smallest positive integer n such that an=e (if it exists)
If no such n 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 H is a subgroup of G, then ∣H∣ divides ∣G∣
The center of a group Z(G) is a subgroup of G and is always abelian
A group G is called simple if it has no proper normal subgroups (subgroups that are invariant under conjugation by elements of G)
The direct product of two groups (G×H,∗) is a group formed by the Cartesian product of the sets G and H with the operation defined component-wise: (a,b)∗(c,d)=(a∗c,b∗d)
Subgroups and Cosets
A subgroup H of a group G must satisfy the following conditions:
H is a non-empty subset of G
For all a,b∈H, a∗b∈H (closure under the group operation)
For all a∈H, a−1∈H (closure under inverses)
The left cosets of a subgroup H in G partition the group G into disjoint sets of equal size
The number of left cosets is called the index of H in G, denoted by [G:H]
The right cosets of a subgroup H in G also partition the group G into disjoint sets of equal size
A subgroup H is called normal if its left and right cosets coincide, i.e., aH=Ha for all a∈G
Normal subgroups are important because they allow for the construction of quotient groups G/H
The kernel of a group homomorphism φ:G→G′ is a normal subgroup of G defined as ker(φ)={a∈G:φ(a)=e′}, where e′ is the identity element of G′
Homomorphisms and Isomorphisms
A group homomorphism is a function φ:G→G′ between two groups that preserves the group structure: φ(a∗b)=φ(a)∗′φ(b) for all a,b∈G, where ∗ and ∗′ are the group operations in G and G′, respectively
The kernel of a homomorphism ker(φ) is always a normal subgroup of the domain group G
The image of a homomorphism Im(φ)={φ(a):a∈G} is a subgroup of the codomain group G′
The first isomorphism theorem states that for a group homomorphism φ:G→G′, the quotient group G/ker(φ) is isomorphic to the image Im(φ)
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) of a group G is the group of all isomorphisms from G 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 G on a vector space V is a group homomorphism ρ:G→GL(V), where GL(V) is the general linear group of invertible linear transformations on V
The dimension of the representation is the dimension of the vector space V
The character of a representation ρ is the function χρ:G→C defined by χρ(g)=tr(ρ(g)), where tr denotes the trace of a matrix
Characters are class functions, i.e., they are constant on conjugacy classes of G
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 G is the representation on the vector space C[G] (the space of complex-valued functions on G) given by the left regular action of G 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 A4 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