3.14. Lecture 14

3.14.1. Induced representations

Let H≤GH\leq G be a subgroup. Given a a representation (π,V)(\pi,V) of HH, we will “stitch together” this with the GG-action on G/HG/H to create a representation of GG, which we call the induced representation of (π,V)(\pi,V). This is often denoted IndHG⁢(π,V)\mathrm{Ind}_{H}^{G}(\pi,V) or (π,V)↑HG(\pi,V)\uparrow_{H}^{G}.

Our definition will depend on a choice of cosets for G/HG/H: let r1,r2,…,rn∈Gr_{1},r_{2},\ldots,r_{n}\in G be such that

G=r1⁢H⊔r2⁢H⊔…⊔rn⁢H;G=r_{1}H\sqcup r_{2}H\sqcup\ldots\sqcup r_{n}H;

here n=|G||H|n=\frac{|G|}{|H|}, and the “rr”s stand for representatives. Note that each g∈Gg\in G may be written uniquely as g=ri⁢hg=r_{i}h for some representative rir_{i} and h∈Hh\in H.

We use these to describe the GG-action on G/HG/H as follows. Define

j⁢(⋅,⋅):G×{1,2,…,n}→{1,2,…,n},h(⋅,⋅):G×{1,2,…,n}→Hj(\cdot,\cdot):G\times\{1,2,\ldots,n\}\rightarrow\{1,2,\ldots,n\},\qquad h_{(% \cdot,\cdot)}:G\times\{1,2,\ldots,n\}\rightarrow H

by the formula

g⁢ri=rj⁢(g,i)⁢h(g,i)gr_{i}=r_{j(g,i)}h_{(g,i)}

for all g∈Gg\in G and i∈{1,…,n}i\in\{1,\ldots,n\}. These functions are well-defined by uniqueness of the decomposition of GG into HH-cosets.

Lemma 3.14.1.
j⁢(g1⁢g2,i)=j⁢(g1,j⁢(g2,i))\displaystyle j(g_{1}g_{2},i)=j\big{(}g_{1},j(g_{2},i)\big{)}
h(g1⁢g2,i)=h(g1,j⁢(g2,i))⁢h(g2,i)\displaystyle h_{(g_{1}g_{2},i)}=h_{\big{(}g_{1},j(g_{2},i)\big{)}}h_{(g_{2},i)}

for all g1,g2∈Gg_{1},g_{2}\in G, i∈{1,…,n}i\in\{1,\ldots,n\}.

Proof.

From the definition of j⁢(⋅,⋅)j(\cdot,\cdot) and h(⋅,⋅)h_{(\cdot,\cdot)}, we have

g1⁢g2⁢ri=rj⁢(g1⁢g2,i)⁢h(g1⁢g2,i).g_{1}g_{2}r_{i}=r_{j(g_{1}g_{2},i)}h_{(g_{1}g_{2},i)}.

On the other hand,

g1⁢g2⁢ri=\displaystyle g_{1}g_{2}r_{i}= g1⁢(g2⁢ri)=g1⁢(rj⁢(g2,i)⁢h(g2,i))=(g1⁢rj⁢(g2,i))⁢h(g2,i)\displaystyle g_{1}(g_{2}r_{i})=g_{1}\big{(}r_{j(g_{2},i)}h_{(g_{2},i)}\big{)}% =\big{(}g_{1}r_{j(g_{2},i)}\big{)}h_{(g_{2},i)}
=(rj⁢(g1,j⁢(g2,i))⁢h(g1,j⁢(g2,i)))⁢h(g2,i)=rj⁢(g1,j⁢(g2,i))⁢(h(g1,j⁢(g2,i))⁢h(g2,i)).\displaystyle=\big{(}r_{j\big{(}g_{1},j(g_{2},i)\big{)}}h_{\big{(}g_{1},j(g_{2% },i)\big{)}}\big{)}h_{(g_{2},i)}=r_{j\big{(}g_{1},j(g_{2},i)\big{)}}\big{(}h_{% \big{(}g_{1},j(g_{2},i)\big{)}}h_{(g_{2},i)}\big{)}.

By uniqueness of the decomposition of GG into HH-cosets, we must then have

rj⁢(g1⁢g2,i)=rj⁢(g1,j⁢(g2,i)),h(g1⁢g2,i)=h(g1,j⁢(g2,i))⁢h(g2,i).r_{j(g_{1}g_{2},i)}=r_{j\big{(}g_{1},j(g_{2},i)\big{)}},\quad h_{(g_{1}g_{2},i% )}=h_{\big{(}g_{1},j(g_{2},i)\big{)}}h_{(g_{2},i)}.

∎

Given a representation (π,V)(\pi,V) of HH and choice of coset representatives 𝐫=(r1,r2,…,rn){\bf r}=(r_{1},r_{2},\ldots,r_{n}) for G/HG/H, we define a vector space

V𝐫=r1⁢V⊕r2⁢V⊕…⊕rn⁢V,V_{{\bf r}}=r_{1}V\oplus r_{2}V\oplus\ldots\oplus r_{n}V,

with vector space operations

α⁢(∑i=1nri⁢𝐯i)+β⁢(∑i=1nri⁢𝐮i):=∑i=1nri⁢(α⁢𝐯i+β⁢𝐮i).\alpha\left(\sum_{i=1}^{n}r_{i}{\bf v}_{i}\right)+\beta\left(\sum_{i=1}^{n}r_{% i}{\bf u}_{i}\right):=\sum_{i=1}^{n}r_{i}(\alpha{\bf v}_{i}+\beta{\bf u}_{i}).
Proposition 3.14.2.

The induced representation IndHG⁢(π,V):=(IndHG⁢π,V𝐫)\mathrm{Ind}_{H}^{G}(\pi,V):=\big{(}\mathrm{Ind}_{H}^{G}\pi,V_{{\bf r}}\big{)} defined by extending the map

IndHG⁢π⁢(g)⁢(ri⁢𝐯):=rj⁢(g,i)⁢π⁢(h(g,i))⁢𝐯\mathrm{Ind}_{H}^{G}\pi(g)\big{(}r_{i}{\bf v}\big{)}:=r_{j(g,i)}\pi(h_{(g,i)})% {\bf v}

linearly to all of V𝐫V_{{\bf r}} (for each g∈Gg\in G) is a representation of GG on V𝐫V_{{\bf r}}.

Proof.

We need to show that IndHG⁢π⁢(g1⁢g2)=IndHG⁢π⁢(g1)⁢IndHG⁢π⁢(g2)\mathrm{Ind}_{H}^{G}\pi(g_{1}g_{2})=\mathrm{Ind}_{H}^{G}\pi(g_{1})\mathrm{Ind}% _{H}^{G}\pi(g_{2}). Let ri⁢𝐯∈V𝐫r_{i}{\bf v}\in V_{{\bf r}}. Then

IndHG⁢π⁢(g1)⁢IndHG⁢π⁢(g2)⁢ri⁢𝐯\displaystyle\mathrm{Ind}_{H}^{G}\pi(g_{1})\mathrm{Ind}_{H}^{G}\pi(g_{2})r_{i}% {\bf v} =IndHG⁢π⁢(g1)⁢rj⁢(g2,i)⁢π⁢(h(g2,i))⁢𝐯\displaystyle=\mathrm{Ind}_{H}^{G}\pi(g_{1})r_{j(g_{2},i)}\pi(h_{(g_{2},i)}){% \bf v}
=rj⁢(g1,j⁢(g2,i))⁢π⁢(h(g1,j⁢(g2,i)))⁢π⁢(h(g2,i))⁢𝐯\displaystyle=r_{j\big{(}g_{1},j(g_{2},i)\big{)}}\pi\big{(}h_{\big{(}g_{1},j(g% _{2},i)\big{)}}\big{)}\pi(h_{(g_{2},i)}){\bf v}
=rj⁢(g1⁢g2,i)⁢π⁢(h(g1⁢g2,i))⁢𝐯\displaystyle=r_{j(g_{1}g_{2},i)}\pi(h_{(g_{1}g_{2},i)}){\bf v}
=IndHG⁢π⁢(g1⁢g2)⁢ri⁢𝐯,\displaystyle=\mathrm{Ind}_{H}^{G}\pi(g_{1}g_{2})r_{i}{\bf v},

where the previous lemma was used for the second-to-last equality. ∎

Remark 3.14.3.

We will later see that making a different choice of coset representatives gives rise to an isomorphic representation.

Example 3.14.4.

Let H=⟨r⟩<DnH=\langle r\rangle<D_{n}. Then Dn=e⁢⟨r⟩⊔s⁢⟨r⟩D_{n}=e\langle r\rangle\sqcup s\langle r\rangle, and H=CnH=C_{n}. Given a representation (ψj,ℂ)(\psi_{j},{\mathbb{C}}), ψj⁢(rk)=e2⁢π⁢i⁢j⁢k/n\psi_{j}(r^{k})=e^{2\pi ijk/n}, we consider the induced representation IndHDn⁢ψj\mathrm{Ind}_{H}^{D_{n}}\psi_{j} on W=e⁢ℂ⊕s⁢ℂW=e{\mathbb{C}}\oplus s{\mathbb{C}}: for z,w∈ℂz,w\in{\mathbb{C}}, we have

IndHDn⁢ψj⁢(s)⁢(e⁢z+s⁢w)=s⁢z+e⁢w,\mathrm{Ind}_{H}^{D_{n}}\psi_{j}(s)(ez+sw)=sz+ew,
IndHDn⁢ψj⁢(r)⁢(e⁢z+s⁢w)=e⁢ψj⁢(r)⁢z+s⁢ψj⁢(r−1)⁢w=e2⁢π⁢i⁢j/n⁢e⁢z+e−2⁢π⁢i⁢j/n⁢s⁢w.\mathrm{Ind}_{H}^{D_{n}}\psi_{j}(r)(ez+sw)=e\psi_{j}(r)z+s\psi_{j}(r^{-1})w=e^% {2\pi ij/n}ez+e^{-2\pi ij/n}sw.

The matrices of these maps with respect to the basis e⁢1e1, s⁢1s1 of WW are then

IndHDn⁢ψj⁢(s)=(0110),IndHDn⁢ψj⁢(r)=(e2⁢π⁢i⁢j/n00e−2⁢π⁢i⁢j/n),\mathrm{Ind}_{H}^{D_{n}}\psi_{j}(s)=\left(\begin{matrix}0&1\\ 1&0\end{matrix}\right),\qquad\mathrm{Ind}_{H}^{D_{n}}\psi_{j}(r)=\left(\begin{% matrix}e^{2\pi ij/n}&0\\ 0&e^{-2\pi ij/n}\end{matrix}\right),

hence

IndHDn⁢(ψj,ℂ)=(ρj,ℂ2).\mathrm{Ind}_{H}^{D_{n}}(\psi_{j},{\mathbb{C}})=(\rho_{j},{\mathbb{C}}^{2}).

Note that dim⁡IndHG⁢π=|G||H|⁢dim⁡π\operatorname{dim}\mathrm{Ind}_{H}^{G}\pi=\frac{|G|}{|H|}\operatorname{dim}\pi.

Recall that since GG acts on G/HG/H, we have the quasi-regular representation (λ,C⁢(G/H))\big{(}\lambda,C(G/H)\big{)}, where C⁢(G/H)={f:G/H→ℂ}C(G/H)=\{f:G/H\rightarrow{\mathbb{C}}\},

[λ⁢(g)⁢f]⁢(g0⁢H)=f⁢(g−1⁢g0⁢H).[\lambda(g)f](g_{0}H)=f(g^{-1}g_{0}H).
Proposition 3.14.5.

(λ,C⁢(G/H))≅IndHG⁢(triv,ℂ)\big{(}\lambda,C(G/H)\big{)}\cong\mathrm{Ind}_{H}^{G}({\mathrm{triv}},{\mathbb% {C}}).

Proof.

We first define T:C⁢(G/H)→ℂ𝐫=r1⁢ℂ⊕…⊕rn⁢ℂT:C(G/H)\rightarrow{\mathbb{C}}_{{\bf r}}=r_{1}{\mathbb{C}}\oplus\ldots\oplus r% _{n}{\mathbb{C}} as follows:

T⁢(f):=r1⁢f⁢(r1⁢H)+r2⁢f⁢(r2⁢H)+…+rn⁢f⁢(rn⁢H).T(f):=r_{1}f(r_{1}H)+r_{2}f(r_{2}H)+\ldots+r_{n}f(r_{n}H).

It is straightforward to verify that this is an invertible linear map, so it remains to show that it is a GG-homomorphism. For g∈Gg\in G and f∈C⁢(G/H)f\in C(G/H),

IndHG⁢triv⁢(g)⁢T⁢(f)=IndHG⁢triv⁢(g)⁢(∑iri⁢f⁢(ri⁢H))=∑irj⁢(g,i)⁢f⁢(ri⁢H).\mathrm{Ind}_{H}^{G}{\mathrm{triv}}(g)T(f)=\mathrm{Ind}_{H}^{G}{\mathrm{triv}}% (g)\left(\sum_{i}r_{i}f(r_{i}H)\right)=\sum_{i}r_{j(g,i)}f(r_{i}H).

Now reparameterising the sum with j=j⁢(g,i)j=j(g,i), hence i=j⁢(g−1,j⁢(g,i))i=j(g^{-1},j(g,i)) (cf. Lemma 3.14.1), we obtain

IndHG⁢triv⁢(g)⁢T⁢(f)=∑jrj⁢f⁢(r(g−1,j)⁢H)=∑jrj⁢f⁢(g−1⁢rj⁢H)=T⁢(λ⁢(g)⁢f).\mathrm{Ind}_{H}^{G}{\mathrm{triv}}(g)T(f)=\sum_{j}r_{j}f(r_{(g^{-1},j)}H)=% \sum_{j}r_{j}f(g^{-1}r_{j}H)=T(\lambda(g)f).

∎

Exercise 3.14.2 generalises this type of isomorphism to any induced representation. We conclude with the following important observation about induced representations:

IndHG⁢π⁢(h)⁢ri⁢𝐯=rj⁢(h,i)⁢π⁢(h(h,i))≠ri⁢π⁢(h)⁢𝐯!\mathrm{Ind}_{H}^{G}\pi(h)r_{i}{\bf v}=r_{j(h,i)}\pi(h_{(h,i)})\neq r_{i}\pi(h% ){\bf v}!

3.14.2. Exercises

.

Problem 81. Let (π,V)(\pi,V) be a representation of H≤GH\leq G. Define

Cπ⁢(G,V)={f:G→V|f⁢(g⁢h)=π⁢(h−1)⁢f⁢(g)⁢∀g∈G,h∈H}.C_{\pi}(G,V)=\{f:G\rightarrow V\,|\,f(gh)=\pi(h^{-1})f(g)\;\forall\;g\in G,\;h% \in H\}.
  1. (a)
    ​

    Compute dim⁡Cπ⁢(G,V)\operatorname{dim}C_{\pi}(G,V).

  2. (b)
    ​

    Show that (λ,Cπ⁢(G,V))\big{(}\lambda,C_{\pi}(G,V)\big{)} is a GG-representation, where as usual [λ⁢(g)⁢f]⁢(g′)=f⁢(g−1⁢g′)[\lambda(g)f](g^{\prime})=f(g^{-1}g^{\prime}) for all g,g′∈Gg,g^{\prime}\in G.

  3. (c)
    ​

    Given a set of representatives 𝐫=r1,…,rn{\bf r}=r_{1},\ldots,r_{n}, let T𝐫:Cπ⁢(G,V)→V𝐫T_{{\bf r}}:C_{\pi}(G,V)\rightarrow V_{{\bf r}} be the map

    T𝐫⁢(f)=r1⁢f⁢(r1)+r2⁢f⁢(r2)+…+rn⁢f⁢(rn).T_{{\bf r}}(f)=r_{1}f(r_{1})+r_{2}f(r_{2})+\ldots+r_{n}f(r_{n}).

    Show that T𝐫T_{{\bf r}} is a GG-isomorphism from (λ,Cπ⁢(G,V))\big{(}\lambda,C_{\pi}(G,V)\big{)} to IndHG⁢(π,V)\mathrm{Ind}_{H}^{G}(\pi,V).

Remark 3.14.6.

This shows that the induced representations of (π,V)(\pi,V) for different choices of representatives for G/HG/H give rise to isomorphic representations!