⭕Groups and Geometries Unit 12 – Finite Group Representation Theory
Finite group representation theory bridges abstract algebra and linear algebra, offering powerful tools to study group structures. It maps group elements to linear transformations, revealing hidden symmetries and properties through characters and irreducible representations.
This theory has wide-ranging applications in physics, chemistry, and mathematics. It simplifies complex problems by exploiting group symmetries, enabling the analysis of molecular vibrations, quantum systems, and geometric structures through character tables and decomposition techniques.
Group consists of a set G together with a binary operation ∗ satisfying closure, associativity, identity, and inverse properties
Representation of a group G is a homomorphism ρ:G→GL(V) where V is a vector space and GL(V) is the general linear group of invertible linear transformations on V
Homomorphism preserves the group structure, i.e., ρ(g1∗g2)=ρ(g1)⋅ρ(g2) for all g1,g2∈G
Character of a representation ρ is the function χρ:G→C defined by χρ(g)=tr(ρ(g)), where tr denotes the trace
Irreducible representation cannot be decomposed into a direct sum of smaller representations
Conjugacy class of an element g∈G is the set {hgh−1:h∈G}
Class function is a function f:G→C that is constant on conjugacy classes, i.e., f(hgh−1)=f(g) for all g,h∈G
Foundations of Group Theory
Subgroup H of a group G is a subset that forms a group under the same operation as G
Cosets of a subgroup H in G are sets of the form gH={gh:h∈H} for g∈G
Cosets partition the group G into disjoint sets of equal size
Normal subgroup N of G satisfies gNg−1=N for all g∈G
Quotient group G/N can be formed by considering cosets of N as elements
Homomorphism φ:G→H is a function that preserves the group operation, i.e., φ(g1∗g2)=φ(g1)⋅φ(g2) for all g1,g2∈G
Kernel of a homomorphism φ is the set ker(φ)={g∈G:φ(g)=eH}, where eH is the identity element of H
Isomorphism is a bijective homomorphism, and isomorphic groups have the same structure
Direct product of groups G and H is the group G×H={(g,h):g∈G,h∈H} with component-wise operation
Introduction to Representation Theory
Representation of a group G on a vector space V is a homomorphism ρ:G→GL(V)
ρ(g) is a linear transformation on V for each g∈G
Degree of a representation is the dimension of the vector space V
Equivalent representations ρ1 and ρ2 satisfy ρ2(g)=A−1ρ1(g)A for some invertible matrix A and all g∈G
Trivial representation maps every group element to the identity transformation
Regular representation is the permutation representation of G acting on itself by left multiplication
Subrepresentation of ρ:G→GL(V) is a representation ρ′:G→GL(W) where W is a subspace of V invariant under ρ(g) for all g∈G
Direct sum of representations ρ1⊕ρ2 acts on the direct sum of the corresponding vector spaces
Characters and Character Tables
Character of a representation ρ is the function χρ:G→C defined by χρ(g)=tr(ρ(g))
Characters are class functions, i.e., constant on conjugacy classes
Character table of a group G is a matrix whose rows correspond to irreducible characters and columns correspond to conjugacy classes
Entries are the values of the irreducible characters on representative elements of each conjugacy class
Orthogonality relations for characters state that irreducible characters are orthonormal with respect to a specific inner product
⟨χi,χj⟩=δij for irreducible characters χi and χj, where δij is the Kronecker delta
Number of irreducible representations equals the number of conjugacy classes
Sum of squares of the degrees of irreducible representations equals the order of the group
Regular character χreg satisfies χreg(e)=∣G∣ and χreg(g)=0 for g=e
Irreducible Representations
Irreducible representation cannot be decomposed into a direct sum of smaller representations
No non-trivial invariant subspaces under the action of the group
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
Consequence: the only matrices that commute with all matrices of an irreducible representation are scalar multiples of the identity
Characters of irreducible representations are orthonormal with respect to the inner product ⟨f,g⟩=∣G∣1∑x∈Gf(x)g(x)
Irreducible characters form a basis for the space of class functions
Number of times an irreducible representation appears in a representation is given by the inner product of their characters
Applications in Geometry
Symmetry group of a geometric object (polygon, polyhedron, etc.) is the group of transformations that leave the object invariant
Representations of the symmetry group can be used to analyze the object's properties
Character theory can be used to determine the number of fixed points of a group action
Burnside's Lemma: the number of orbits is the average number of fixed points over all group elements
Representations can be used to construct symmetric and antisymmetric tensors
Symmetric tensors are invariant under permutations of indices, while antisymmetric tensors change sign under odd permutations
Invariant theory studies polynomials that are invariant under a group action
Molien series is a generating function that encodes the dimensions of the spaces of invariant polynomials of each degree
Representation theory can be used to analyze the vibrations and normal modes of molecules and crystals
Symmetry-adapted linear combinations of atomic orbitals form basis functions for irreducible representations
Problem-Solving Techniques
Determine the conjugacy classes and the size of each class
Elements in the same conjugacy class have the same character values
Construct the character table by calculating the traces of representative matrices for each conjugacy class
Use orthogonality relations to check the table's consistency
Decompose a representation into irreducible representations using the inner product of characters
Multiply the character of the representation by each irreducible character and divide by the group order
Apply Schur's Lemma to determine the structure of commutant algebras and intertwining maps
Commutant algebra consists of matrices that commute with all matrices of the representation
Use Molien's theorem to find the generating function for the dimensions of invariant polynomial spaces
Substitute the character values into the Molien series formula
Utilize Burnside's Lemma to count the number of orbits under a group action
Calculate the average number of fixed points over all group elements
Advanced Topics and Extensions
Projective representations are homomorphisms from a group to the projective general linear group PGL(V)
Useful for studying groups with nontrivial cohomology, such as the symmetric group Sn for n≥4
Unitary representations are representations where the matrices ρ(g) are unitary, i.e., ρ(g)−1=ρ(g)†
Unitary representations are important in quantum mechanics and harmonic analysis
Lie groups are continuous groups with a smooth manifold structure
Representations of Lie groups are crucial in theoretical physics and harmonic analysis
Induced representations are constructed by starting with a representation of a subgroup and extending it to the whole group
Frobenius reciprocity relates induced representations to restricted representations
Modular representation theory studies representations over fields of positive characteristic
Decomposition of representations can be more complicated due to the presence of non-semisimple modules
Categorification of representation theory replaces vector spaces with categories and linear maps with functors
Provides a deeper understanding of representation-theoretic concepts and connections to other areas of mathematics