🧩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.
Induced representations construct a representation of a group G from a representation of a subgroup H
Let H be a subgroup of G and (ρ,V) a representation of H
The induced representation (IndHGρ,IndHGV) is a representation of G
Induction is a functor from the category of H-modules to the category of G-modules
Frobenius reciprocity relates the induction functor to the restriction functor
Restriction functor takes a G-module and views it as an H-module
Transitive G-sets correspond to cosets of subgroups (orbits under the action of G)
Induction preserves irreducibility in certain cases (Mackey's irreducibility criterion)
Subgroups and Quotient Groups
A subgroup H of a group G is a subset that is closed under the group operation and inverses
The left cosets of H in G are the sets gH={gh:h∈H} for each g∈G
Right cosets are defined similarly as Hg={hg:h∈H}
The set of left cosets forms a partition of G and is denoted G/H
If H is a normal subgroup, the set of cosets G/H has a natural group structure (quotient group)
The index of H in G, denoted [G:H], is the number of distinct left (or right) cosets
Lagrange's theorem states that for a finite group G, the order of any subgroup H divides the order of G
The order of G is equal to the product of the order of H and the index [G:H]
Construction of Induced Representations
Let H be a subgroup of G and (ρ,V) a representation of H
The induced representation IndHGV is the vector space of functions f:G→V satisfying f(hg)=ρ(h)f(g) for all h∈H,g∈G
The group G acts on this space by left translation: (gf)(x)=f(g−1x)
Choose a set of representatives {gi} for the left cosets of H in G
For each gi, define a function fi:G→V by fi(gj)=δijv for some fixed v∈V
The set {fi} forms a basis for IndHGV
The dimension of IndHGV is equal to [G:H]⋅dimV
Properties of Induced Representations
Induction is transitive: if K≤H≤G, then IndKG≅IndHG∘IndKH
Induction preserves direct sums: IndHG(V⊕W)≅IndHGV⊕IndHGW
Induction is left adjoint to restriction: HomG(IndHGV,W)≅HomH(V,ResHGW) (Frobenius reciprocity)
Mackey's formula relates induced representations from different subgroups
For subgroups H,K≤G, ResKGIndHG≅⨁g∈K\G/HIndK∩gHg−1KResK∩gHg−1gHg−1gρ
Induced representations can be used to construct irreducible representations (Mackey's irreducibility criterion)
If ResHGρ is irreducible and ResgHg−1Gρ≆ResgHg−1Ggρ for all g∈/H, then IndHGρ is irreducible
Frobenius Reciprocity
Frobenius reciprocity is a fundamental result relating induction and restriction of representations
It states that for a subgroup H≤G and representations (ρ,V) of H and (π,W) of G, there is a natural isomorphism:
HomG(IndHGV,W)≅HomH(V,ResHGW)
This isomorphism is given by the map ϕ↦ϕe, where ϕe(v)=ϕ(fv)(e) and fv(g)=ρ(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, where hi=gi−1ggi
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)=∣H∣1∑h∈Hχρ(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=S3 and H={e,(12)}. Compute the induced representation of the trivial representation of H.
Show that the regular representation of a finite group G is isomorphic to the induced representation of the trivial representation of the trivial subgroup.
Let G=D4 (dihedral group of order 8) and H={e,r2}. Compute the character table of G using induced representations.
Prove that if H is a subgroup of index 2 in G, then IndHGC≅C⊕C−, where C− is the sign representation of G.
Let G=S4 and H=S3 (as a subgroup fixing one element). Decompose the permutation representation of G on C4 into irreducible representations using Frobenius reciprocity.
Compute the induced representation of the standard representation of S2 to S3.
Decompose this representation into irreducible components.
Let G=GL(2,C) and B be the subgroup of upper triangular matrices. Compute the character of the induced representation of the determinant character of B.