Groups and Geometries

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.

Key Concepts and Definitions

  • Group consists of a set GG together with a binary operation * satisfying closure, associativity, identity, and inverse properties
  • Representation of a group GG is a homomorphism ρ:GGL(V)\rho: G \rightarrow GL(V) where VV is a vector space and GL(V)GL(V) is the general linear group of invertible linear transformations on VV
    • Homomorphism preserves the group structure, i.e., ρ(g1g2)=ρ(g1)ρ(g2)\rho(g_1 * g_2) = \rho(g_1) \cdot \rho(g_2) for all g1,g2Gg_1, g_2 \in G
  • Character of a representation ρ\rho is the function χρ:GC\chi_\rho: G \rightarrow \mathbb{C} defined by χρ(g)=tr(ρ(g))\chi_\rho(g) = \text{tr}(\rho(g)), where tr\text{tr} denotes the trace
  • Irreducible representation cannot be decomposed into a direct sum of smaller representations
  • Conjugacy class of an element gGg \in G is the set {hgh1:hG}\{hgh^{-1} : h \in G\}
  • Class function is a function f:GCf: G \rightarrow \mathbb{C} that is constant on conjugacy classes, i.e., f(hgh1)=f(g)f(hgh^{-1}) = f(g) for all g,hGg, h \in G

Foundations of Group Theory

  • Subgroup HH of a group GG is a subset that forms a group under the same operation as GG
  • Cosets of a subgroup HH in GG are sets of the form gH={gh:hH}gH = \{gh : h \in H\} for gGg \in G
    • Cosets partition the group GG into disjoint sets of equal size
  • Normal subgroup NN of GG satisfies gNg1=NgNg^{-1} = N for all gGg \in G
    • Quotient group G/NG/N can be formed by considering cosets of NN as elements
  • Homomorphism φ:GH\varphi: G \rightarrow H is a function that preserves the group operation, i.e., φ(g1g2)=φ(g1)φ(g2)\varphi(g_1 * g_2) = \varphi(g_1) \cdot \varphi(g_2) for all g1,g2Gg_1, g_2 \in G
    • Kernel of a homomorphism φ\varphi is the set ker(φ)={gG:φ(g)=eH}\text{ker}(\varphi) = \{g \in G : \varphi(g) = e_H\}, where eHe_H is the identity element of HH
  • Isomorphism is a bijective homomorphism, and isomorphic groups have the same structure
  • Direct product of groups GG and HH is the group G×H={(g,h):gG,hH}G \times H = \{(g, h) : g \in G, h \in H\} with component-wise operation

Introduction to Representation Theory

  • Representation of a group GG on a vector space VV is a homomorphism ρ:GGL(V)\rho: G \rightarrow GL(V)
    • ρ(g)\rho(g) is a linear transformation on VV for each gGg \in G
  • Degree of a representation is the dimension of the vector space VV
  • Equivalent representations ρ1\rho_1 and ρ2\rho_2 satisfy ρ2(g)=A1ρ1(g)A\rho_2(g) = A^{-1}\rho_1(g)A for some invertible matrix AA and all gGg \in G
  • Trivial representation maps every group element to the identity transformation
  • Regular representation is the permutation representation of GG acting on itself by left multiplication
  • Subrepresentation of ρ:GGL(V)\rho: G \rightarrow GL(V) is a representation ρ:GGL(W)\rho': G \rightarrow GL(W) where WW is a subspace of VV invariant under ρ(g)\rho(g) for all gGg \in G
  • Direct sum of representations ρ1ρ2\rho_1 \oplus \rho_2 acts on the direct sum of the corresponding vector spaces

Characters and Character Tables

  • Character of a representation ρ\rho is the function χρ:GC\chi_\rho: G \rightarrow \mathbb{C} defined by χρ(g)=tr(ρ(g))\chi_\rho(g) = \text{tr}(\rho(g))
    • Characters are class functions, i.e., constant on conjugacy classes
  • Character table of a group GG 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\langle \chi_i, \chi_j \rangle = \delta_{ij} for irreducible characters χi\chi_i and χj\chi_j, where δij\delta_{ij} 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\chi_{\text{reg}} satisfies χreg(e)=G\chi_{\text{reg}}(e) = |G| and χreg(g)=0\chi_{\text{reg}}(g) = 0 for geg \neq 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=1GxGf(x)g(x)\langle f, g \rangle = \frac{1}{|G|} \sum_{x \in G} f(x)\overline{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)PGL(V)
    • Useful for studying groups with nontrivial cohomology, such as the symmetric group SnS_n for n4n \geq 4
  • Unitary representations are representations where the matrices ρ(g)\rho(g) are unitary, i.e., ρ(g)1=ρ(g)\rho(g)^{-1} = \rho(g)^\dagger
    • 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


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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.