3 Induced representations

3.5 Mackey’s formula — nonexaminable

We want to come up with a criterion for IndHGχ to be irreducible. This is equivalent to

IndHGχ,IndHGχG=1

which is in turn equivalent, by Frobenius reciprocity, to

ResHGIndHGχ,χH=1.

So we try to solve the more general problem of decomposing ResHGIndHGV, as a representation of H. In fact, we will solve the more general problem of finding

ResHGIndKGV

for H and K arbitrary subgroups of G.

3.5.1 Double cosets

Let G be a group and let H,K be subgroups. A double coset HgK is a set of the form

HgK={hgk:hH,kK}.

Like cosets, any two double cosets are either equal or disjoint, so they partition the group. Unlike cosets, they do not have to have the same size. A sequence g1,,gr such that G is the disjoint union

G=i=1rHgiK

is called a set of double coset representatives for H and K in G. We write H\G/K for the set of double cosets of H and K in G.

Lemma 3.17.

The double cosets HgK are the in bijection with the orbits of H acting on G/K.

Proof.

Two cosets gK and gK are in the same H-orbit, if and only if hgK=gK for some hH, if and only if

HgK=HgK.

So we have a bijection which takes the double coset HgK to the H-orbit of gK. ∎

Example 3.18.

Let H=K=Sn-1G=Sn, n3, thinking of H as the set of elements that fix the number n. Then H=HeH is one double coset. I claim that G=HH(n-1n)H. Indeed, a complete set of left coset representatives for H in G is

{e,(1n),(2n),,((n-1)n)}.

As I can write (in)=(in-1)(n-1n)(in-1)H(n-1n)H for in-1, we see that the left cosets (1n)H,,(n-1n)H are all contained in the same double coset H(n-1n)H, as required.

This may be clearer from the orbits point of view. There is a bijection G/H{1,,n} which respects the action of G — the bijection takes gH to g(n). The orbits of H=Sn-1 acting on {1,,n} are {n} and {1,,n-1}, which gives the two double cosets.

If sK is a left coset of K, we write Hs=HsKs-1; note that this is independent of choice of representative s. The notation is motivated by the fact that Hs is the stabiliser of sK for the action of H on G/K discussed above. This leads to the following lemma.

Lemma 3.19.

If sG, then as a disjoint union of cosets of K we have

HsK=h1sKh2sKhrsK

where h1,,hr are a complete set of left coset representatives for Hs in H.

3.5.2 Mackey’s formula

Suppose that KG, that sG, and that (ρ,V) is a representation of K. Then we can define a representation (ρs,V) of Hs=sHs-1 by taking Vs=V (same vector space) and ρs(h)=ρ(s-1hs) for hHs.

Theorem 3.20.

(Mackey’s formula) Let H,K be subgroups of G and let (ρ,V) be a representation of K. Let s1,,sr be a set of double coset representatives for H and K in G.

Then

ResHGIndKGVs{s1,,sr}IndHsHResHsKsVs.
Proof.

Let g1,,gn be the left coset representatives for K in G. Then

IndKGV=g1VgnV.

The action of H permutes the giV among themselves, with giV and gjV in the same H-orbit if and only if HgiK=HgjK. Therefore for each double coset HsK we have an H-subrepresentation

Ws=i:giKHsKgiV.

Now, by lemma 3.19 above, these gi have the form his for hi a set of left coset representatives for Hs in H. From the decomposition

Ws=hiHsH/HshisV

we see that

WsIndHsHsV.

It remains to show that sV, as a representation of Hs, is isomorphic to Vs. The map VssV taking v to sv is the required isomorphism, because

ρ(h)(sv)=ρ(h)ρ(s)v=ρ(s)ρ(s-1hs)v=sρs(h)v.

3.5.3 Irreducibility criterion

Theorem 3.21.

Let ρ be an irreducible representation of HG. Then IndHGρ is irreducible if and only if, for every g in a set of double coset representatives of H\G/H, with gH,

HomHg(ρ,ρg)=0

where Hg=HgHg-1.

Proof.

Indeed, let S=g0,,gr be such a set of double coset representatives, with g0H. By Mackey’s formula and Frobenius reciprocity,

IndHGρ,IndHGρG =ρ,ResHGIndHGρH
=ρ,gSIndHgHρgH
=ρ,ρH+g{g1,,gr}ρ,IndHgHρgH
=ρ,ρH+g{g1,,gr}ρ,ρgHg.

Since ρ is irreducible, the first term on the right is equal to 1 and all the other terms are at least 0. So

IndHGρ,IndHGρG1

with equality if and only if HomHg(ρ,ρg)=0 for all gSH. The result follows. ∎

Corollary 3.22.

If HG and ρ is an irreducible representation of H, then

IndHGρ

is irreducible if and only if ρ≇ρg for all g in a set of coset representatives of H in G with gH.

Proof.

If H is normal, then double cosets, left cosets, and right cosets are all the same. For gG, ρg is another irreducible representation of H so

HomH(ρ,ρg)0

if and only if ρ≇ρg. ∎

3.5.4 Mackey examples

Example 3.23.

Let G=DnH=Cn. Let χ:Cn× with χ(r)=ω. The previous corollary shows that

IndHGχ

is reducible if and only if χχs. But

χs(r)=χ(s-1rs)=χ(r-1)=ω-1.

So IndHGχ is irreducible if and only if ωω-1 (which we already knew).

Example 3.24.

Let ρ be an irreducible representation of Sn-1Sn with character χ. Then {e,s} is a set of double coset representatives for Sn-1 in Sn, where s=(n-1n). We have

Sn-1sSn-1=Sn-2

of elements fixing n-1 and n.

Moreover, χsχ (because elements of Sn-2 are conjugate in Sn-2 if and only if they are conjugate in Sn-1, so they have the same character!) and so we see

IndSn-1Snχ,IndSn-1Snχ =χ,χSn-1+χ,χSn-2
=1+χ,χSn-2.

For example, if χ is the degree 2 irreducible character of S4, then χ|S3 is still irreducible so the right hand side of this formula gives two. And indeed,

IndS4S5χ=ψ+ψϵ

where ψ is one of the irreducible five-dimensional representations of S5.

3.5.5 Index two

Let G be a group and let H be a subgroup of index two (necessarily normal). Let sG with sH. Let ϵ:G× be the unique (order two) character with kernel H.

Of course, we have in mind the example H=An, G=Sn.

Theorem 3.25.

Suppose that ρ is an irreducible representation of H. Then

  1. 1.

    if ρρs, then

    IndHGρσϵσ

    for some irreducible representation σ of G with ResHGσρ.

  2. 2.

    if ρ≇ρs, then

    σ=IndHGρ

    is irreducible, with σϵσ.

Proof.

Let ρ have character χ. By the normal subgroup case of Mackey’s theorem,

IndHGχ,IndHGχG=1+χ,χsH.

It follows that the induction IndHGχ is irreducible if and only if χχs. This gives the second statement, and most of the first (we leave the proof that, in all cases, IndHGχϵIndHGχ as an exercise.)

If χ=χs, then we have IndHGχ=ψ+ψ for some irreducible characters ψ and ψ of G. Restricting to H, we have ψ|H+ψ|H=2χ so that ψ extends χ. But then we have

IndHGχ=IndHGResHGψ=ψ(IndHG𝟙)=ψ(𝟙+ϵ)=ψ+ϵψ

so that IndHGχ=ψ+ϵψ as required. ∎