Representation Theory

🧩Representation Theory Unit 6 – Induced Representations

Induced representations are a powerful tool in representation theory, allowing us to construct representations of larger groups from those of smaller subgroups. This technique bridges the gap between local and global symmetries, providing insights into group structure and behavior. Understanding induced representations is crucial for applications in physics and chemistry. They help describe symmetries in quantum systems, classify vibrational modes of molecules, and play a role in particle physics and quantum field theory. Mastering this concept opens doors to advanced topics in mathematical physics.

Key Concepts and Definitions

  • Induced representations construct a representation of a group GG from a representation of a subgroup HH
  • Let HH be a subgroup of GG and (ρ,V)(\rho, V) a representation of HH
  • The induced representation (IndHGρ,IndHGV)(\text{Ind}_H^G \rho, \text{Ind}_H^G V) is a representation of GG
  • Induction is a functor from the category of HH-modules to the category of GG-modules
  • Frobenius reciprocity relates the induction functor to the restriction functor
    • Restriction functor takes a GG-module and views it as an HH-module
  • Transitive GG-sets correspond to cosets of subgroups (orbits under the action of GG)
  • Induction preserves irreducibility in certain cases (Mackey's irreducibility criterion)

Subgroups and Quotient Groups

  • A subgroup HH of a group GG is a subset that is closed under the group operation and inverses
  • The left cosets of HH in GG are the sets gH={gh:hH}gH = \{gh : h \in H\} for each gGg \in G
    • Right cosets are defined similarly as Hg={hg:hH}Hg = \{hg : h \in H\}
  • The set of left cosets forms a partition of GG and is denoted G/HG/H
  • If HH is a normal subgroup, the set of cosets G/HG/H has a natural group structure (quotient group)
  • The index of HH in GG, denoted [G:H][G:H], is the number of distinct left (or right) cosets
  • Lagrange's theorem states that for a finite group GG, the order of any subgroup HH divides the order of GG
    • The order of GG is equal to the product of the order of HH and the index [G:H][G:H]

Construction of Induced Representations

  • Let HH be a subgroup of GG and (ρ,V)(\rho, V) a representation of HH
  • The induced representation IndHGV\text{Ind}_H^G V is the vector space of functions f:GVf: G \to V satisfying f(hg)=ρ(h)f(g)f(hg) = \rho(h)f(g) for all hH,gGh \in H, g \in G
    • The group GG acts on this space by left translation: (gf)(x)=f(g1x)(gf)(x) = f(g^{-1}x)
  • Choose a set of representatives {gi}\{g_i\} for the left cosets of HH in GG
  • For each gig_i, define a function fi:GVf_i: G \to V by fi(gj)=δijvf_i(g_j) = \delta_{ij}v for some fixed vVv \in V
    • The set {fi}\{f_i\} forms a basis for IndHGV\text{Ind}_H^G V
  • The dimension of IndHGV\text{Ind}_H^G V is equal to [G:H]dimV[G:H] \cdot \dim V

Properties of Induced Representations

  • Induction is transitive: if KHGK \leq H \leq G, then IndKGIndHGIndKH\text{Ind}_K^G \cong \text{Ind}_H^G \circ \text{Ind}_K^H
  • Induction preserves direct sums: IndHG(VW)IndHGVIndHGW\text{Ind}_H^G(V \oplus W) \cong \text{Ind}_H^G V \oplus \text{Ind}_H^G W
  • Induction is left adjoint to restriction: HomG(IndHGV,W)HomH(V,ResHGW)\text{Hom}_G(\text{Ind}_H^G V, W) \cong \text{Hom}_H(V, \text{Res}_H^G W) (Frobenius reciprocity)
  • Mackey's formula relates induced representations from different subgroups
    • For subgroups H,KGH, K \leq G, ResKGIndHGgK\G/HIndKgHg1KResKgHg1gHg1gρ\text{Res}_K^G \text{Ind}_H^G \cong \bigoplus_{g \in K \backslash G / H} \text{Ind}_{K \cap gHg^{-1}}^K \text{Res}_{K \cap gHg^{-1}}^{gHg^{-1}} {}^g\rho
  • Induced representations can be used to construct irreducible representations (Mackey's irreducibility criterion)
    • If ResHGρ\text{Res}_H^G \rho is irreducible and ResgHg1GρResgHg1Ggρ\text{Res}_{gHg^{-1}}^G \rho \ncong \text{Res}_{gHg^{-1}}^G {}^g\rho for all gHg \notin H, then IndHGρ\text{Ind}_H^G \rho is irreducible

Frobenius Reciprocity

  • Frobenius reciprocity is a fundamental result relating induction and restriction of representations
  • It states that for a subgroup HGH \leq G and representations (ρ,V)(\rho, V) of HH and (π,W)(\pi, W) of GG, there is a natural isomorphism:
    • HomG(IndHGV,W)HomH(V,ResHGW)\text{Hom}_G(\text{Ind}_H^G V, W) \cong \text{Hom}_H(V, \text{Res}_H^G W)
  • This isomorphism is given by the map ϕϕe\phi \mapsto \phi_e, where ϕe(v)=ϕ(fv)(e)\phi_e(v) = \phi(f_v)(e) and fv(g)=ρ(g1)vf_v(g) = \rho(g^{-1})v
  • Frobenius reciprocity allows for the computation of intertwining numbers between induced and restricted representations
  • It is a key tool in the study of the representation theory of finite groups and Lie algebras
  • Frobenius reciprocity can be generalized to the context of modules over algebras (adjunction between induction and restriction functors)

Applications in Physics and Chemistry

  • Induced representations play a crucial role in the study of symmetry in quantum mechanics
  • The symmetry group of a quantum system determines its allowed energy levels and transitions
    • Irreducible representations correspond to energy eigenspaces
  • Crystal field theory uses induced representations to describe the splitting of atomic orbitals in transition metal complexes
    • The symmetry of the ligand environment induces a representation of the point group on the d-orbitals
  • Vibrational modes of molecules can be classified using induced representations of the molecular point group
  • The Poincaré group, the symmetry group of special relativity, has physically relevant induced representations (e.g., spin representations)
  • Induced representations of the Lorentz group are used in the classification of elementary particles
  • In quantum field theory, the construction of interacting theories often involves induced representations of the gauge group

Computational Techniques

  • Computation of induced representations can be done using the formula IndHGρ(g)=iρ(hi)egi\text{Ind}_H^G \rho(g) = \sum_i \rho(h_i) \otimes e_{g_i}, where hi=gi1ggih_i = g_i^{-1}gg_i
  • The matrix elements of the induced representation can be computed using a set of coset representatives
  • Character theory provides a way to decompose induced representations into irreducible components
    • The character of an induced representation is given by the induced character formula: χIndHGρ(g)=1HhHχρ(hgh1)\chi_{\text{Ind}_H^G \rho}(g) = \frac{1}{|H|} \sum_{h \in H} \chi_\rho(hgh^{-1})
  • Mackey's formula can be used to compute the restriction of an induced representation to a subgroup
  • Computation of intertwining numbers and Frobenius reciprocity can be done using character inner products
  • The Littlewood-Richardson rule gives a combinatorial method for decomposing tensor products of induced representations of symmetric groups
  • Computational algebra systems (e.g., GAP, Magma) have built-in functions for working with induced representations

Examples and Practice Problems

  • Let G=S3G = S_3 and H={e,(12)}H = \{e, (1 2)\}. Compute the induced representation of the trivial representation of HH.
  • Show that the regular representation of a finite group GG is isomorphic to the induced representation of the trivial representation of the trivial subgroup.
  • Let G=D4G = D_4 (dihedral group of order 8) and H={e,r2}H = \{e, r^2\}. Compute the character table of GG using induced representations.
  • Prove that if HH is a subgroup of index 2 in GG, then IndHGCCC\text{Ind}_H^G \mathbb{C} \cong \mathbb{C} \oplus \mathbb{C}^-, where C\mathbb{C}^- is the sign representation of GG.
  • Let G=S4G = S_4 and H=S3H = S_3 (as a subgroup fixing one element). Decompose the permutation representation of GG on C4\mathbb{C}^4 into irreducible representations using Frobenius reciprocity.
  • Compute the induced representation of the standard representation of S2S_2 to S3S_3.
    • Decompose this representation into irreducible components.
  • Let G=GL(2,C)G = GL(2, \mathbb{C}) and BB be the subgroup of upper triangular matrices. Compute the character of the induced representation of the determinant character of BB.


© 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.

© 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.