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Frobenius Theorem

Mounir Lbath, March 2024

Table of Contents

  1. The Frobenius Theorem
  2. Representations of a Finite Group
  3. Characters
  4. Induced Representations
  5. Proof of the Frobenius Theorem
  6. Appendix: Useful Prerequisites

Introduction

The theory of representations of finite groups, discovered by Frobenius toward the end of the 19th century, consists in analyzing the properties and structure of a finite group (G,⋅)(G, \cdot) by making it act linearly on a vector space. In this post, we use representation theory to prove a theorem about Frobenius groups. In the appendix, we gather some prerequisites that we will use without further mention in this text. This work was originally a TIPE (Travail d'Initiative Personnelle Encadré) for the Ecole Normale Supérieure and was given the grade 18/20.


The Frobenius Theorem

Definition 1.
Let (G,⋅)(G, \cdot) be a finite group with identity ee and HH a proper subgroup of GG (i.e. H≠{e}H \neq \{e\} and H≠GH \neq G). We say that GG is a Frobenius group, that HH is a Frobenius complement, and that (G,H)(G,H) is a Frobenius pair if

∀ g∈G∖H,gHg−1∩H={e}.\forall\, g\in G\setminus H,\quad gHg^{-1}\cap H=\{e\}.

Note that this is equivalent to

∀ (x,y)∈G2,y−1x∉H  ⟹  xHx−1∩yHy−1={e}.\forall\, (x,y)\in G^2,\quad y^{-1}x\notin H\implies xHx^{-1}\cap yHy^{-1}=\{e\}.

Intuitively, this means that the conjugates of HH cover GG "as much as possible."

Proposition 1.
If (G,H)(G,H) is a Frobenius pair, then

∣⋃g∈GgHg−1∣=∣G∣+1−∣G∣∣H∣.\Bigl|\bigcup_{g\in G} gHg^{-1}\Bigr| = |G|+1-\frac{|G|}{|H|}.

Proof.
We have

∣⋃g∈GgHg−1∣=∣{e} ⊔ ⨆gH∈G/H(gHg−1∖{e})∣=1+∣G/H∣(∣H∣−1).□\Bigl|\bigcup_{g\in G} gHg^{-1}\Bigr| = \Bigl|\{e\}\,\sqcup\,\bigsqcup_{gH\in G/H}\Bigl(gHg^{-1}\setminus\{e\}\Bigr)\Bigr| = 1 + |G/H|(|H|-1). \square

One can show that for any subgroup HH the above equality is in fact an inequality (≤)(\leq). It also shows that the conjugates of a proper subgroup never cover GG (recall that GG is finite, otherwise G=GLn(C)G=GL_n(\mathbb{C}) and H=Tn(C)∩GLn(C)H=T_n(\mathbb{C})\cap GL_n(\mathbb{C}) the group of invertible triangular matrices produce a counter-example).

Example 1.
Let GG be a finite group acting transitively on a set XX such that for every g∈G∖{e}g\in G\setminus\{e\}, gg fixes at most one point of XX. Then, if α∈X\alpha\in X is such that Stab⁡(α)≠{e}\operatorname{Stab}(\alpha)\neq\{e\}, the pair (G,Stab⁡(α))(G,\operatorname{Stab}(\alpha)) is a Frobenius pair.

Proof.
We have Stab⁡(α)≠G\operatorname{Stab}(\alpha)\neq G (by transitivity). If g∈G∖Stab⁡(α)g\in G\setminus\operatorname{Stab}(\alpha), then g⋅α≠αg\cdot\alpha\neq\alpha; hence g⋅αg\cdot\alpha and α\alpha are simultaneously fixed only by ee. Therefore, Stab⁡(g⋅α)∩Stab⁡(α)={e}\operatorname{Stab}(g\cdot\alpha)\cap \operatorname{Stab}(\alpha)=\{e\}, i.e. g Stab⁡(α) g−1∩Stab⁡(α)={e}g\,\operatorname{Stab}(\alpha)\,g^{-1}\cap\operatorname{Stab}(\alpha)=\{e\} □\square.

One can in fact show that every Frobenius group is of this form. Here are some examples:

Example 2.

  • If KK is a finite field and G=Aff⁡(1,K)={τa,b:x∈K↦ax+b, (a,b)∈K∗×K}G=\operatorname{Aff}(1,K)=\{\tau_{a,b}: x\in K\mapsto ax+b,\ (a,b)\in K^*\times K\} is the group of affine bijections of KK onto itself, and H(K)={τa,0:x∈K↦ax, a∈K∗}H(K)=\{\tau_{a,0}: x\in K\mapsto ax,\ a\in K^*\} (the subgroup of those that fix 00), then (G,H)(G,H) is a Frobenius pair. (Note: τa,b\tau_{a,b} fixes exactly b/(1−a)b/(1-a) for a≠1a\neq1; fixes no point of KK for a=1a=1 and b≠0b\neq0; and fixes all of KK for a=1a=1 and b=0b=0 — i.e. for τa,b=id\tau_{a,b}=\mathrm{id}; finally, H(K)=Stab⁡(0)H(K)=\operatorname{Stab}(0).)
  • If G=A4G=A_4 (the alternating group) and γ\gamma is a 3-cycle, then (G,⟨γ⟩)(G,\langle \gamma\rangle) is a Frobenius pair.
  • If n∈N∗n\in\mathbb{N}^* is odd, DnD_n is the dihedral group (the group of affine transformations of the plane preserving the regular nn-gon centered at the origin), and ss is an orthogonal symmetry in DnD_n, then (Dn,⟨s⟩)(D_n,\langle s\rangle) is a Frobenius pair.

Theorem 1 (Frobenius).
Let (G,H)(G,H) be a Frobenius pair. Define

N=(G∖(⋃g∈GgHg−1))∪{e},N=\Bigl(G\setminus\bigl(\bigcup_{g\in G}gHg^{-1}\bigr)\Bigr)\cup\{e\},

called the Frobenius kernel. Then NN is a normal subgroup of GG, and N∩H={e}N\cap H=\{e\}, and G=NHG=NH (we say that GG is the semidirect product of NN by HH).

The fact that N∩H={e}N\cap H=\{e\} is evident; moreover, by Proposition 1,

∣N∣=∣G∣−∣⋃g∈GgHg−1∣+1=∣G∣∣H∣.|N|=|G|-\Bigl|\bigcup_{g\in G}gHg^{-1}\Bigr|+1=\frac{|G|}{|H|}.

Assuming that NN is a subgroup of GG, the map

φ:(n,h)∈N×H↦nh\varphi: (n,h)\in N\times H\mapsto nh

is injective (if nh=n′h′nh=n'h' then n′−1n=h′h−1∈N∩H={e}n'^{-1}n=h'h^{-1}\in N\cap H=\{e\}, hence (n,h)=(n′,h′)(n,h)=(n',h')) and, by cardinality, surjective; thus, G=NHG=NH. Moreover, if g∈Gg\in G, then gNg−1⊆NgNg^{-1}\subseteq N (otherwise an element of N∖{e}N\setminus\{e\} would be conjugate to an element of HH, contradicting the definition of NN); hence, NN is normal. The difficult part of the theorem lies in proving that NN is a subgroup. This will be demonstrated in Section 5.

Example 3.
Revisiting the pairs from Example 2 in the “group action” formulation of Example 1, the Frobenius kernel is the set of elements of GG acting without fixed points, to which the identity ee is added. Thus:

  • The kernel of (A4,⟨γ⟩)(A_4,\langle \gamma\rangle) is the Klein group V={id, (1 2)(3 4), (1 3)(2 4), (1 4)(2 3)}.V=\{\mathrm{id},\,(1\,2)(3\,4),\,(1\,3)(2\,4),\,(1\,4)(2\,3)\}.
  • The kernel of (Aff⁡(1,K),H(K))(\operatorname{Aff}(1,K),H(K)) is the subgroup {τ1,b:b∈K}\{\tau_{1,b}:b\in K\} of translations in Aff⁡(1,K)\operatorname{Aff}(1,K).
  • The Frobenius kernel of DnD_n is the group of rotations centered at the origin by an angle in 2πnZ\frac{2\pi}{n}\mathbb{Z} (naturally isomorphic to UnU_n).

Representations of a Finite Group

To prove the Frobenius theorem, we will try to express NN as the kernel of a representation.

Definition 2.
Let (G,⋅)(G,\cdot) be a finite group. A representation of GG is a pair (ρ,V)(\rho,V) where VV is a finite-dimensional C\mathbb{C}-vector space and ρ\rho is a homomorphism from GG to GL⁡(V)\operatorname{GL}(V). We will sometimes denote it simply by ρ\rho. The degree of ρ\rho is the integer dim⁡(V)\dim(V).

Thus, we view the elements of GG as linear transformations on VV.

Example 4.

  • Representations of degree 1 correspond to homomorphisms from GG to C∗\mathbb{C}^*. In particular, the trivial representation is the one corresponding to the trivial homomorphism from GG to C∗\mathbb{C}^*.
  • A more elaborate example: if (fg)g∈G(f_g)_{g\in G} is a basis of a vector space VV of dimension ∣G∣|G| indexed by GG, and for each g∈Gg\in G we define ρ(g)\rho(g) as the unique element of GL⁡(V)\operatorname{GL}(V) such that ∀ h∈G,ρ(g)(fh)=fgh,\forall\, h\in G,\quad \rho(g)(f_h)=f_{gh}, then we have defined a representation of GG called the regular representation. Moreover, it is said to be faithful because ker⁡(ρ)={e}\ker(\rho)=\{e\}.
  • If (ρ,V)(\rho,V) and (ρ′,V′)(\rho',V') are two representations of GG, then by setting, for g∈Gg\in G, one defines a representation on the space L(V,V′)L(V,V') (the space of linear maps from VV to V′V') by ∀ u∈L(V,V′),(ρ,ρ′~)(g)(u)=ρ′(g)∘u∘ρ(g−1).\forall\, u\in L(V,V'),\quad (\widetilde{\rho,\rho'})(g)(u)=\rho'(g)\circ u\circ \rho(g^{-1}).
  • Let (ρ,V)(\rho,V) and (ρ′,V′)(\rho',V') be as above. Then one defines a representation (ρ⊕ρ′, V⊕V′)(\rho\oplus\rho',\,V\oplus V') by ∀ (g,v,v′)∈G×V×V′,(ρ⊕ρ′)(g)((v,v′))=(ρ(g)(v), ρ′(g)(v′)).\forall\,(g,v,v')\in G\times V\times V',\quad (\rho\oplus\rho')(g)((v,v'))=(\rho(g)(v),\,\rho'(g)(v')). This construction also works for direct sum decompositions in which ρ\rho and ρ′\rho' are defined: in a basis adapted to this decomposition, the matrices of (ρ⊕ρ′)(g)(\rho\oplus\rho')(g) will consist of two square diagonal blocks of sizes dim⁡(V)\dim(V) and dim⁡(V′)\dim(V').

Definition 3.
If (ρ,V)(\rho,V) and (ρ′,V′)(\rho',V') are two representations of GG, we say that ρ\rho is equivalent to ρ′\rho' (and write ρ∼ρ′\rho\sim\rho') if dim⁡(V)=dim⁡(V′)\dim(V)=\dim(V') and if there exist bases ee of VV and e′e' of V′V' such that

∀ g∈G,Mat⁡(ρ(g))=Mat⁡(ρ′(g)).\forall\, g\in G,\quad \operatorname{Mat}(\rho(g))=\operatorname{Mat}(\rho'(g)).

In other words, if there exists an isomorphism u∈L(V,V′)u\in L(V,V') such that

∀ g∈G,u∘ρ(g)=ρ′(g)∘u.\forall\, g\in G,\quad u\circ \rho(g)=\rho'(g)\circ u.

Moreover, for any ρ,ρ′\rho,\rho' we denote

Hom⁡(ρ,ρ′)={u∈L(V,V′)∣∀ g∈G,  u∘ρ(g)=ρ′(g)∘u},\operatorname{Hom}(\rho,\rho')=\{u\in L(V,V')\mid \forall\, g\in G,\; u\circ \rho(g)=\rho'(g)\circ u\},

which is clearly a subspace of L(V,V′)L(V,V').

Definition 4.
A representation ρ\rho of GG is said to be irreducible if the only subspaces of VV that are stable under all ρ(g)\rho(g) for g∈Gg\in G are {0}\{0\} and VV.

These representations cannot be “broken” into subrepresentations; this is the case, for example, for representations of degree 1. In fact, we have the following proposition:

Proposition 2 (Maschke).
Let (ρ,V)(\rho,V) be a representation of GG and UU a subspace of VV that is stable under all ρ(g)\rho(g) for g∈Gg\in G. Then there exists a supplementary subspace SS of UU that is also stable under all ρ(g)\rho(g).

Proof.
It suffices to construct a projector with image UU that commutes with all ρ(g)\rho(g); its kernel will then be the desired supplementary subspace. Let pp be any projector with image UU. Modify it by averaging over GG:

q=1∣G∣∑g∈Gρ(g)∘p∘ρ(g−1).q=\frac{1}{|G|}\sum_{g\in G}\rho(g)\circ p\circ \rho(g^{-1}).

This is an endomorphism whose image is contained in UU and such that q∣U=id⁡Uq|_U=\operatorname{id}_U (since the ρ(g)\rho(g) stabilize UU) and which commutes with all ρ(g)\rho(g) (because ρ(g)∘q∘ρ(g−1)=q\rho(g)\circ q\circ \rho(g^{-1})=q, as the map g↦hgg\mapsto hg is bijective). □\square

By induction on the dimension of VV, one shows the following reduction result:

Proposition 3.
If (ρ,V)(\rho,V) is a representation, then there exists k∈N∗k\in\mathbb{N}^* and subspaces V1,V2,…,VkV_1,V_2,\dots,V_k of VV such that

V=⨁i=1kVi,V=\bigoplus_{i=1}^k V_i,

and there exist irreducible representations (ρ1,V1),…,(ρk,Vk)(\rho_1,V_1),\dots,(\rho_k,V_k) such that

ρ=ρ1⊕ρ2⊕⋯⊕ρk.\rho=\rho_1\oplus\rho_2\oplus\cdots\oplus\rho_k.

Finally, here is one last proposition that will prove very useful:

Proposition 4 (Schur).
Let (ρ,V)(\rho,V) and (ρ′,V′)(\rho',V') be two irreducible representations of GG. Then dim⁡Hom⁡(ρ,ρ′)={1if ρ∼ρ′,0if ρ≁ρ′.\dim\operatorname{Hom}(\rho,\rho')= \begin{cases} 1 & \text{if } \rho\sim\rho', \\[1mm] 0 & \text{if } \rho\not\sim\rho'. \end{cases}

Proof.

  • Suppose ρ∼ρ′\rho\sim\rho'. Up to transporting ρ′\rho' via the isomorphism given by the equivalence, assume V=V′V=V' and ρ=ρ′\rho=\rho'. Let u∈Hom⁡(ρ,ρ)u\in\operatorname{Hom}(\rho,\rho). Since C\mathbb{C} is algebraically closed, uu has an eigenvalue λ\lambda. Then for all g∈Gg\in G, uu and ρ(g)\rho(g) commute, hence the eigenspace Eλ(u)=ker⁡(u−λ id⁡)E_\lambda(u)=\ker(u-\lambda\,\operatorname{id}) is stable under ρ(g)\rho(g). By the irreducibility of ρ\rho, since Eλ(u)E_\lambda(u) is nonzero, it must equal VV, so that u=λ id⁡u=\lambda\,\operatorname{id}. Conversely, every map of the form λ id⁡\lambda\,\operatorname{id} (with λ∈C\lambda\in\mathbb{C}) belongs to Hom⁡(ρ,ρ)\operatorname{Hom}(\rho,\rho). Hence, Hom⁡(ρ,ρ)=C id⁡\operatorname{Hom}(\rho,\rho)=\mathbb{C}\,\operatorname{id} has dimension 1.
  • Suppose ρ≁ρ′\rho\not\sim\rho'. Let u∈Hom⁡(ρ,ρ′)u\in\operatorname{Hom}(\rho,\rho'). For any g∈Gg\in G, we have ρ′(g)∘u=u∘ρ(g)\rho'(g)\circ u=u\circ \rho(g). Thus, the image im⁡(u)\operatorname{im}(u) is stable under ρ′(g)\rho'(g). By irreducibility, im⁡(u)\operatorname{im}(u) is either V′V' or {0}\{0\}. Similarly, ker⁡(u)\ker(u) is either VV or {0}\{0\}. Therefore, if uu is not an isomorphism, then ker⁡(u)=V\ker(u)=V and im⁡(u)={0}\operatorname{im}(u)=\{0\}, so that u=0u=0. This completes the proof. □\square

Characters

A large part of the information contained in a representation is actually stored in its character:

Definition 5.
Let (ρ,V)(\rho,V) be a representation of GG. The character of ρ\rho is the function

χρ:G→C,g↦Tr⁡(ρ(g)).\chi_\rho: G\to\mathbb{C},\quad g\mapsto \operatorname{Tr}(\rho(g)).

A character is any function in CG\mathbb{C}^G that is the character of some representation. We say that a character is irreducible if it comes from an irreducible representation.

Example 5.

  • χ(e)=Tr⁡(id⁡)\chi(e)=\operatorname{Tr}(\operatorname{id}) is the degree of the representation.
  • Two equivalent representations have the same character (i.e. the same matrices in well-chosen bases).
  • If g,h∈Gg,h\in G and χ\chi is a character, then χ(ghg−1)=Tr⁡(ρ(g)ρ(h)ρ(g)−1)=Tr⁡(ρ(h))=χ(h).\chi(ghg^{-1})=\operatorname{Tr}\bigl(\rho(g)\rho(h)\rho(g)^{-1}\bigr)=\operatorname{Tr}(\rho(h))=\chi(h). We denote by Cent⁡(G)\operatorname{Cent}(G) the subspace of central functions on GG (i.e. functions constant on the conjugacy classes of GG; its dimension is the number of such classes). Then χ∈Cent⁡(G)\chi\in\operatorname{Cent}(G).
  • Trivially, χρ1⊕ρ2=χρ1+χρ2\chi_{\rho_1\oplus\rho_2}=\chi_{\rho_1}+\chi_{\rho_2}.
  • For any g∈Gg\in G, since g∣G∣=eg^{|G|}=e, the polynomial X∣G∣−1=∏ω∈U∣G∣(X−ω)X^{|G|}-1=\prod_{\omega\in U_{|G|}}(X-\omega) annihilates ρ(g)\rho(g) and splits with simple roots. Hence, ρ(g)\rho(g) is diagonalizable with spectrum contained in U∣G∣U_{|G|}. If {λ1,…,λd}\{\lambda_1,\dots,\lambda_d\} is the spectrum of ρ(g)\rho(g), then {λ1−1,…,λd−1}\{\lambda_1^{-1},\dots,\lambda_d^{-1}\} is the spectrum of ρ(g)−1=ρ(g−1),\rho(g)^{-1}=\rho(g^{-1}), so that, since the eigenvalues lie in U∣G∣U_{|G|}, χ(g−1)=λ1−1+⋯+λd−1=λ1+⋯+λd‾=χ(g)‾.\chi(g^{-1})=\lambda_1^{-1}+\cdots+\lambda_d^{-1}=\overline{\lambda_1+\cdots+\lambda_d}=\overline{\chi(g)}.
  • Using the notations of Example 4, one has χ(ρ,ρ′~)=χρ‾,χρ′,\chi_{(\widetilde{\rho,\rho'})}=\overline{\chi_{\rho}},\chi_{\rho'}, which is a consequence (via the previous point and the definition of (ρ,ρ′~)(\widetilde{\rho,\rho'})) of the fact that for A,B∈Mn(C)A,B\in M_n(\mathbb{C}), the linear map M∈Mn(C)↦AMB∈Mn(C)M\in M_n(\mathbb{C})\mapsto AMB\in M_n(\mathbb{C}) has trace Tr⁡(A)Tr⁡(B)\operatorname{Tr}(A)\operatorname{Tr}(B).

Definition/Proposition 1.
We endow CG\mathbb{C}^G with the Hermitian inner product (see Appendix) defined by

∀ (u,v)∈CG×CG,⟨u,v⟩=1∣G∣∑g∈Gu(g)‾v(g).\forall\,(u,v)\in\mathbb{C}^G\times\mathbb{C}^G,\quad \langle u,v\rangle=\frac{1}{|G|}\sum_{g\in G} \overline{u(g)}v(g).

To compute the Hermitian inner product of two characters, we again use the “averaging technique”:

Lemma 1.
Let ρ\rho be a representation. Then

1∣G∣∑g∈Gρ(g)\frac{1}{|G|}\sum_{g\in G}\rho(g)

is a projector onto

VG:=⋂g∈Gker⁡(ρ(g)−id⁡).V_G:=\bigcap_{g\in G}\ker\Bigl(\rho(g)-\operatorname{id}\Bigr).

Proof.
If x∈VGx\in V_G, then

1∣G∣∑g∈Gρ(g)(x)=1∣G∣∑g∈Gx=x(1).\frac{1}{|G|}\sum_{g\in G}\rho(g)(x)=\frac{1}{|G|}\sum_{g\in G}x=x\quad (1).

Moreover, if x∈Vx\in V and

y=1∣G∣∑g∈Gρ(g)(x),y=\frac{1}{|G|}\sum_{g\in G}\rho(g)(x),

then for any h∈Gh\in G

ρ(h)(y)=1∣G∣∑g∈Gρ(hg)(x)=y,\rho(h)(y)=\frac{1}{|G|}\sum_{g\in G}\rho(hg)(x)=y,

(since the map g↦hgg\mapsto hg is bijective) hence y∈VGy\in V_G (2).

With (1) and (2), the result follows. □\square

Proposition 5.
If (ρ,V)(\rho,V) and (ρ′,V′)(\rho',V') are two representations of GG, then

⟨χρ,χρ′⟩=dim⁡Hom⁡(ρ,ρ′).\langle\chi_\rho,\chi_{\rho'}\rangle=\dim\operatorname{Hom}(\rho,\rho').

Proof.
Define (ρ,ρ′~)(\widetilde{\rho,\rho'}) as in Example 4. Apply Lemma 1 to this representation.

On one hand,

⋂g∈Gker⁡((ρ,ρ′~)(g)−id⁡L(V,V′))=Hom⁡(ρ,ρ′),\bigcap_{g\in G}\ker\Bigl((\widetilde{\rho,\rho'})(g)-\operatorname{id}_{L(V,V')}\Bigr)=\operatorname{Hom}(\rho,\rho'),

so that

Tr⁡(1∣G∣∑g∈G(ρ,ρ′~)(g))=dim⁡Hom⁡(ρ,ρ′),\operatorname{Tr}\Bigl(\frac{1}{|G|}\sum_{g\in G}(\widetilde{\rho,\rho'})(g)\Bigr)=\dim\operatorname{Hom}(\rho,\rho'),

(since for a projector its trace equals its rank). On the other hand, by linearity and Example 5,

Tr⁡(1∣G∣∑g∈G(ρ,ρ′~)(g))=1∣G∣∑g∈Gχ(ρ,ρ′~)(g)=1∣G∣∑g∈Gχρ(g)‾χρ′(g)=⟨χρ,χρ′⟩.\operatorname{Tr}\Bigl(\frac{1}{|G|}\sum_{g\in G}(\widetilde{\rho,\rho'})(g)\Bigr)=\frac{1}{|G|}\sum_{g\in G}\chi_{(\widetilde{\rho,\rho'})}(g) =\frac{1}{|G|}\sum_{g\in G} \overline{\chi_\rho(g)}\chi_{\rho'}(g)=\langle\chi_\rho,\chi_{\rho'}\rangle.

Combining with Schur’s lemma (Proposition 4) completes the proof. □\square

Corollary 1.
If (ρ,V)(\rho,V) and (ρ′,V′)(\rho',V') are two irreducible representations of GG, then

⟨χρ,χρ′⟩={1if ρ∼ρ′,0if ρ≁ρ′.\langle\chi_\rho,\chi_{\rho'}\rangle= \begin{cases} 1 & \text{if } \rho\sim\rho',\\[1mm] 0 & \text{if } \rho\not\sim\rho'. \end{cases}

Thus, the family of irreducible characters is orthonormal and finite (since CG\mathbb{C}^G is finite-dimensional). Moreover, two non-equivalent irreducible representations have distinct characters; hence there are as many irreducible representations (up to equivalence) as there are irreducible characters.

Denote by ρ1,…,ρr\rho_1,\dots,\rho_r a complete set of irreducible representations and by χ1,…,χr\chi_1,\dots,\chi_r the associated characters. Combining with Proposition 3, we obtain:

Corollary 2.
If ρ\rho is a representation, then there exist (n1,…,nr)∈Nr(n_1,\dots,n_r)\in\mathbb{N}^r such that

ρ∼n1ρ1⊕⋯⊕nrρr(where niρi denotes ρi⊕⋯⊕ρi (ni times)).\rho\sim n_1\rho_1\oplus\cdots\oplus n_r\rho_r\quad (\text{where } n_i\rho_i \text{ denotes } \rho_i\oplus\cdots\oplus\rho_i \text{ ($n_i$ times)}).

Then the character of ρ\rho is given by

χ=∑i=1rniχi.\chi=\sum_{i=1}^r n_i\chi_i.

Proposition 6.
If ρ\rho and ρ′\rho' are two representations, then

ρ∼ρ′  ⟺  χρ=χρ′.\rho\sim\rho'\iff\chi_\rho=\chi_{\rho'}.

Proof.
The direct implication is clear. Suppose χρ=χρ′=:χ\chi_\rho=\chi_{\rho'}=: \chi. Write

ρ∼n1ρ1⊕⋯⊕nrρrandρ′∼n1′ρ1⊕⋯⊕nr′ρr.\rho\sim n_1\rho_1\oplus\cdots\oplus n_r\rho_r\quad \text{and}\quad \rho'\sim n'_1\rho_1\oplus\cdots\oplus n'_r\rho_r.

By orthonormality, ∑j=1rnj⟨χi,χj⟩=ni\sum_{j=1}^r n_j\langle\chi_i,\chi_j\rangle=n_i and similarly ⟨χi,χρ′⟩=ni′\langle\chi_i,\chi_{\rho'}\rangle=n'_i. Thus, ni=ni′n_i=n'_i for each ii, and so ρ∼ρ′\rho\sim\rho'. □\square

One can in fact show a stronger result than the orthonormality of characters (we will not prove it here):

Proposition 7.
The irreducible characters χ1,…,χr\chi_1,\dots,\chi_r form an orthonormal basis of Cent⁡(G)\operatorname{Cent}(G). Thus, rr is the number of conjugacy classes in GG and if f∈Cent⁡(G)f\in\operatorname{Cent}(G),

f=∑i=1r⟨χi,f⟩χi.f=\sum_{i=1}^r\langle\chi_i,f\rangle\chi_i.

Induced Representations

Let HH be a subgroup of GG. Starting from a representation (ρ,V)(\rho,V) of GG, one can easily obtain the representation (ρ∣H,V)(\rho|_H,V) of HH, denoted ρ∣H\rho|_H. Conversely, the purpose of this section is to give a natural way to extend a representation (ρ0,W)(\rho_0,W) of HH to a representation (ρ,V)(\rho,V) of GG (with W⊆VW\subseteq V). Denote

G=⨆i=1lgiH,G=\bigsqcup_{i=1}^l g_iH,

the partition of GG into left cosets modulo HH (with g1H=Hg_1H=H).

Definition 6.
Let (ρ,V)(\rho,V) be a representation of GG and let WW be a subspace of VV that is stable under ρ(h)\rho(h) for all h∈Hh\in H. Let ρ0=ρ∣H,W\rho_0=\rho|_{H,W} be the restriction of ρ\rho to HH and the subspace WW. We say that ρ\rho is induced from ρ0\rho_0 and write

ρ=Ind⁡HG(ρ0)\rho=\operatorname{Ind}^G_H(\rho_0)

if

V=⨁i=1lρ(gi)(W).(*)V=\bigoplus_{i=1}^l \rho(g_i)(W).\tag{*}

Note that under the assumptions of Definition 6, if g∈Gg\in G can be written as g=gihg=g_i h with h∈Hh\in H, then

ρ(g)(W)=ρ(gih)(W)=ρ(gi)∘ρ(h)(W)=ρ(gi)(W).\rho(g)(W)=\rho(g_i h)(W)=\rho(g_i)\circ \rho(h)(W)=\rho(g_i)(W).

Thus, the subspaces ρ(gi)(W)\rho(g_i)(W) do not depend on the choice of representatives of the left cosets modulo HH. We have the following proposition:

Proposition 8.
If ρ′\rho' is a representation of HH, there exists (up to equivalence) a unique representation ρ\rho of GG such that

ρ=Ind⁡HG(ρ′).\rho=\operatorname{Ind}^G_H(\rho').

We do not prove this (although the proof is quite strait-forward once you read the following): let's just observe that if (ρ0,W)(\rho_0,W) and the action of the ρ(gi)\rho(g_i) on WW are fixed, then the induced representation is uniquely determined. Indeed, it is enough that it be so on the subspaces ρ(gi)(W)\rho(g_i)(W) (by direct sum) and if g∈Gg\in G, 1≤i≤l1\le i\le l, w∈Ww\in W, one has

ρ(g)(ρ(gi)(w))=ρ(gj)(ρ0(h)(w))\rho(g)(\rho(g_i)(w))=\rho(g_j)(\rho_0(h)(w))

where g gi=gjhg\,g_i=g_jh (we take the representative of the class of g gig\,g_i modulo HH).

Proposition 9.
Let (ρ,V)(\rho,V) and (ρ′,V′)(\rho',V') be two representations of GG and let (ρ0,W)(\rho_0,W) be a representation of HH. Suppose that ρ=Ind⁡HG(ρ0)\rho=\operatorname{Ind}^G_H(\rho_0) (in particular, ρ0=ρ∣H,W\rho_0=\rho|_{H,W}). Then

Hom⁡(ρ,ρ′)≃Hom⁡(ρ0,ρ′∣H).\operatorname{Hom}(\rho,\rho')\simeq \operatorname{Hom}(\rho_0,\rho'|_H).

Proof.
The map

u∈Hom⁡(ρ,ρ′)⊂L(V,V′)⟼u∣W∈Hom⁡(ρ0,ρ′∣H)⊂L(W,V′)u\in\operatorname{Hom}(\rho,\rho')\subset L(V,V')\longmapsto u|_W\in \operatorname{Hom}(\rho_0,\rho'|_H)\subset L(W,V')

is linear. For bijectivity, one shows that any element v∈Hom⁡(ρ0,ρ′∣H)v\in \operatorname{Hom}(\rho_0,\rho'|_H) extends uniquely to an element u∈Hom⁡(ρ,ρ′)u\in\operatorname{Hom}(\rho,\rho') on VV via the direct sum decomposition (*). □\square

Translating Proposition 9 into an equality of dimensions (using Proposition 5), we have:

Corollary 3.
Using the notations of Proposition 9 and denoting Ind⁡HG(χρ0)=χρ\operatorname{Ind}^G_H(\chi_{\rho_0})=\chi_\rho, and letting ⟨ ⋅ ,⋅ ⟩G\langle\,\cdot\,,\cdot\,\rangle_G (resp. ⟨ ⋅ ,⋅ ⟩H\langle\,\cdot\,,\cdot\,\rangle_H) be the canonical inner product on Cent⁡(G)\operatorname{Cent}(G) (resp. Cent⁡(H)\operatorname{Cent}(H)), we have

⟨Ind⁡HG(χρ0),χρ′⟩G=⟨χρ0,χρ′∣H⟩H.\langle\operatorname{Ind}^G_H(\chi_{\rho_0}),\chi_{\rho'}\rangle_G=\langle\chi_{\rho_0},\chi_{\rho'}|_H\rangle_H.

Thus, by Proposition 6, one may speak of the "induced character" of χρ0\chi_{\rho_0} for Ind⁡HG(χρ0)\operatorname{Ind}^G_H(\chi_{\rho_0}).

Proposition 10.
If χ\chi is a character of HH, then for every g∈Gg\in G,

Ind⁡HG(χ)(g)=1∣H∣∑k∈Gkgk−1∈Hχ(kgk−1).\operatorname{Ind}^G_H(\chi)(g)=\frac{1}{|H|}\sum_{\substack{k\in G\\kgk^{-1}\in H}} \chi(kgk^{-1}).

Proof.
Let (ρ,V)(\rho,V) and (ρ′,W)(\rho',W) be such that χ=χρ′\chi=\chi_{\rho'} and ρ=Ind⁡HG(ρ′)\rho=\operatorname{Ind}^G_H(\rho'). For g∈Gg\in G, ρ(g)\rho(g) permutes the subspaces ρ(gi)(W)\rho(g_i)(W). In a basis adapted to the decomposition

V=⨁i=1lρ(gi)(W),V=\bigoplus_{i=1}^l \rho(g_i)(W),

to compute the trace of ρ(g)\rho(g) it suffices to consider those indices ii such that

ρ(g)(ρ(gi)(W))=ρ(gi)(W),\rho(g)(\rho(g_i)(W))=\rho(g_i)(W),

i.e. such that gi−1ggi∈Hg_i^{-1}gg_i\in H. Thus, by the invariance of trace under change of basis (transporting ρ(gi)(W)\rho(g_i)(W) to WW via the isomorphism ρ(gi)\rho(g_i)),

χ(g)=∑1≤i≤lgi−1ggi∈HTr⁡(ρ(g)∣ρ(gi)(W))=∑1≤i≤lgi−1ggi∈HTr⁡(ρ(gi−1ggi)∣W)=∑1≤i≤lgi−1ggi∈Hχ(gi−1ggi).\chi(g)=\sum_{\substack{1\le i\le l\\ g_i^{-1}gg_i\in H}} \operatorname{Tr}(\rho(g)|_{\rho(g_i)(W)}) =\sum_{\substack{1\le i\le l\\ g_i^{-1}gg_i\in H}} \operatorname{Tr}(\rho(g_i^{-1}gg_i)|_W) =\sum_{\substack{1\le i\le l\\ g_i^{-1}gg_i\in H}} \chi(g_i^{-1}gg_i).

Since χ\chi is central on HH and each right coset of HH has cardinality ∣H∣|H|, the result follows. □\square

This formula allows us to define Ind⁡HG(f)\operatorname{Ind}^G_H(f) for any central function ff (replacing χ\chi by ff in the formula). As the characters linearly generate the central functions, we deduce from Corollary 3:

Proposition 11.
If f1∈Cent⁡(H)f_1\in\operatorname{Cent}(H) and f2∈Cent⁡(G)f_2\in\operatorname{Cent}(G), then

⟨Ind⁡HG(f1),f2⟩G=⟨f1,f2∣H⟩H.\langle \operatorname{Ind}^G_H(f_1), f_2\rangle_G=\langle f_1, f_2|_H\rangle_H.

Proof of the Frobenius Theorem

Now we present the proof of Theorem 1. Fix a Frobenius pair (G,H)(G,H). Let NN be the corresponding Frobenius kernel. The central result in the proof is the following proposition:

Proposition 12.
Let χ\chi be an irreducible character of HH. There exists an irreducible character χ~\widetilde{\chi} of GG such that χ~∣H=χ\widetilde{\chi}|_H=\chi and χ~\widetilde{\chi} is constant on NN.

Remark 1.
It is easy to see that any central function on HH extends in a unique way to a central function on GG which is constant on NN. What matters here is that this extension is a (irreducible) character.

Here is a lemma that will allow us to produce characters constant on NN:

Lemma 2.
Let f∈Cent⁡(H)f\in\operatorname{Cent}(H) such that f(e)=0f(e)=0 and let f~=Ind⁡HG(f)\widetilde{f}=\operatorname{Ind}^G_H(f). Then f~∣H=f\widetilde{f}|_H=f and f~∣N=0\widetilde{f}|_N=0.

Proof.
It is immediate from the definition of the induced function that f~(e)=0=f(e)\widetilde{f}(e)=0=f(e).
Let g∈H∖{e}g\in H\setminus\{e\}. Note that if k∈Gk\in G then kgk−1∈Hkgk^{-1}\in H if and only if g∈k−1Hk∩Hg\in k^{-1}Hk\cap H. By the definition of a Frobenius complement, k∈Hk\in H. Hence,

f~(g)=1∣H∣∑k∈Gkgk−1∈Hf(kgk−1)=1∣H∣∑k∈Hf(kgk−1)=1∣H∣⋅∣H∣⋅f(g)=f(g).\widetilde{f}(g)=\frac{1}{|H|}\sum_{\substack{k\in G\\kgk^{-1}\in H}} f(kgk^{-1}) =\frac{1}{|H|}\sum_{k\in H} f(kgk^{-1}) =\frac{1}{|H|}\cdot|H|\cdot f(g)=f(g).

Now, let g∈N∖{e}g\in N\setminus\{e\}. For any k∈Gk\in G, kgk−1∉Hkgk^{-1}\notin H (otherwise g∈k−1Hkg\in k^{-1}Hk, contradicting the definition of NN), thus f~(g)=0\widetilde{f}(g)=0. □\square

Proof of Proposition 12.
Let d=χ(e)d=\chi(e) be the degree of χ\chi, l=∣G∣/∣H∣∈Nl=|G|/|H|\in\mathbb{N}, θH\theta_H the trivial character of HH and θG\theta_G the trivial character of GG. If χ\chi is the trivial character, simply take χ~\widetilde{\chi} as the trivial character of GG, which is irreducible.

Otherwise, to apply Lemma 2, consider χ−d⋅θH∈Cent⁡(H)\chi-d\cdot \theta_H\in\operatorname{Cent}(H) which vanishes at ee.

Then, set

ψ~:=Ind⁡HG(χ−d⋅θH).\widetilde{\psi}:=\operatorname{Ind}^G_H(\chi-d\cdot\theta_H).

By Lemma 2, ψ~\widetilde{\psi} vanishes on NN and restricts to χ−d⋅θH\chi-d\cdot\theta_H on HH (denoted by (∗)(*)). However, ψ~\widetilde{\psi} is not a character (since ψ~(e)=0\widetilde{\psi}(e)=0). In order to obtain an irreducible character, we need a central function of Hermitian norm 1. Compute, using Proposition 11,

⟨ψ~,ψ~⟩G=⟨Ind⁡HG(χ−d⋅θH),ψ~⟩G=⟨χ−d⋅θH,ψ~∣H⟩H=⟨χ−d⋅θH,χ−d⋅θH⟩H=1+d2,\langle\widetilde{\psi},\widetilde{\psi}\rangle_G=\langle \operatorname{Ind}^G_H(\chi-d\cdot\theta_H),\widetilde{\psi}\rangle_G =\langle\chi-d\cdot\theta_H,\widetilde{\psi}|_H\rangle_H =\langle\chi-d\cdot\theta_H,\chi-d\cdot\theta_H\rangle_H=1+d^2,

(using the orthonormality of irreducible characters and the fact that χ≠θH\chi\neq\theta_H). Also, by Proposition 11,

⟨ψ~,θG⟩G=⟨Ind⁡HG(χ−d⋅θH),θG⟩G=⟨χ−d⋅θH,θG∣H⟩H=⟨χ−d⋅θH,θH⟩H=−d.\langle\widetilde{\psi},\theta_G\rangle_G=\langle \operatorname{Ind}^G_H(\chi-d\cdot\theta_H),\theta_G\rangle_G =\langle\chi-d\cdot\theta_H,\theta_G|_H\rangle_H=\langle\chi-d\cdot\theta_H,\theta_H\rangle_H=-d.

Thus, we set

χ~=ψ~+d⋅θG.\widetilde{\chi}=\widetilde{\psi}+d\cdot\theta_G.

Then, using the inner products in Cent⁡(G)\operatorname{Cent}(G),

⟨χ~,χ~⟩=⟨ψ~,ψ~⟩+2d⟨ψ~,θG⟩+d2⟨θG,θG⟩=1+d2−2d2+d2=1.\langle\widetilde{\chi},\widetilde{\chi}\rangle=\langle\widetilde{\psi},\widetilde{\psi}\rangle+2d\langle\widetilde{\psi},\theta_G\rangle+d^2\langle\theta_G,\theta_G\rangle = 1+d^2-2d^2+d^2=1.

Moreover, χ~\widetilde{\chi} is clearly a Z\mathbb{Z}-linear combination of characters. Hence, there exist integers n1,…,nrn_1,\dots,n_r such that

χ~=∑i=1rniχi.\widetilde{\chi}=\sum_{i=1}^r n_i\chi_i.

Then

1=⟨χ~,χ~⟩=n12+⋯+nr2,1=\langle\widetilde{\chi},\widetilde{\chi}\rangle=n_1^2+\cdots+n_r^2,

so that, as the nin_i are integers, only one of them is nonzero and equals ±1\pm1. Since χ~(e)=d>0\widetilde{\chi}(e)=d>0, that nonzero nin_i equals 1 and χ~\widetilde{\chi} is an irreducible character.

Finally, χ~\widetilde{\chi} remains constant on NN (because we added d⋅θGd\cdot\theta_G to ψ~\widetilde{\psi}, which was constant on NN), and for h∈Hh\in H,

χ~(h)=ψ~(h)+d⋅θG(h)=(χ−d⋅θH)(h)+d=χ(h).\widetilde{\chi}(h)=\widetilde{\psi}(h)+d\cdot\theta_G(h) =(\chi-d\cdot\theta_H)(h)+d =\chi(h).

Thus, χ~∣H=χ\widetilde{\chi}|_H=\chi, which completes the proof. □\square

Remark 2.
We actually know all the values taken by χ~\widetilde{\chi}. Indeed, one has

G=N∪(⋃g∈GgHg−1),G=N\cup \Bigl(\bigcup_{g\in G}gHg^{-1}\Bigr),

and no element of NN is conjugate to an element of ⋃g∈GgHg−1∖{e}\bigcup_{g\in G}gHg^{-1}\setminus\{e\} (otherwise it would be conjugate to an element of H∖{e}H\setminus\{e\}). Moreover, every element of ⋃g∈GgHg−1∖{e}\bigcup_{g\in G}gHg^{-1}\setminus\{e\} is conjugate to an element of HH. If we denote by A1,…,AmA_1,\dots,A_m the conjugacy classes in GG of the elements of ⋃g∈GgHg−1∖{e}\bigcup_{g\in G}gHg^{-1}\setminus\{e\}, then

⋃g∈GgHg−1∖{e}=⨆i=1mAi,\bigcup_{g\in G}gHg^{-1}\setminus\{e\}=\bigsqcup_{i=1}^m A_i,

and we choose h1∈A1∩H,…,hm∈Am∩Hh_1\in A_1\cap H,\dots, h_m\in A_m\cap H. Then, since characters are central, one obtains the following table:

eeA1A_1…\dotsAmA_mN∖{e}N\setminus\{e\}
ψ~\widetilde{\psi}00χ(h1)−d\chi(h_1)-d…\dotsχ(hm)−d\chi(h_m)-d00
θG\theta_G1111…\dots1111
χ~=ψ~+dθG\widetilde{\chi}=\widetilde{\psi}+d\theta_Gddχ(h1)\chi(h_1)…\dotsχ(hm)\chi(h_m)dd

(with d=χ(e)=χ~(e)d=\chi(e)=\widetilde{\chi}(e)).

The decomposition of a character into irreducible characters yields the following corollary:

Corollary 4.
Let χ\chi be a character of HH. There exists a character χ~\widetilde{\chi} of GG such that χ~∣H=χ\widetilde{\chi}|_H=\chi and χ~\widetilde{\chi} is constant on NN. The table above remains valid.

One last lemma will allow us to conclude.

Lemma 3.
Let χ\chi be a character of GG coming from a representation ρ\rho. Then

χ(g)=χ(e)if and only ifg∈ker⁡(ρ).\chi(g)=\chi(e)\quad\text{if and only if}\quad g\in\ker(\rho).

Proof.
Let d=χ(e)d=\chi(e) be the degree of ρ\rho. For g∈Gg\in G, as seen in Example 5, ρ(g)\rho(g) is diagonalizable with spectrum {λ1,…,λd}\{\lambda_1,\dots,\lambda_d\} in UU. Then by the triangle inequality,

∣χ(g)∣=∣λ1+⋯+λd∣≤∣λ1∣+⋯+∣λd∣=d=χ(e),|\chi(g)|=|\lambda_1+\cdots+\lambda_d|\le|\lambda_1|+\cdots+|\lambda_d|=d=\chi(e),

with equality if and only if λ1,…,λd\lambda_1,\dots,\lambda_d are positively collinear, i.e. if they are all equal (since they are of modulus 1). Therefore, χ(g)=χ(e)\chi(g)=\chi(e) if and only if λ1=⋯=λd=1\lambda_1=\cdots=\lambda_d=1, that is, if and only if ρ(g)=id⁡\rho(g)=\operatorname{id}. □\square

At this point, all the ingredients are in place to conclude.

Conclusion of the Proof of Theorem 1.
Take ρ\rho a faithful representation of HH (for example, the regular representation) and χ\chi its character. Let χ~\widetilde{\chi} be as in Corollary 4 and ρ~\widetilde{\rho} the associated representation. We now show that

N=ker⁡(ρ~).N=\ker(\widetilde{\rho}).

From the table in Remark 2 and Lemma 3, we have

ker⁡(ρ~)={x∈G∣χ~(x)=χ~(e)}=N,\ker(\widetilde{\rho})=\{x\in G\mid \widetilde{\chi}(x)=\widetilde{\chi}(e)\}=N,

(where the last equality uses the fact that for the chosen h1,…,hmh_1,\dots,h_m we have χ(hi)≠χ(e)\chi(h_i)\neq\chi(e) by Lemma 3 and the faithfulness of ρ\rho).

Thus, NN is indeed a (normal) subgroup of GG, which completes the proof.

□\huge\square


Appendix: Useful Prerequisites

In this section, let (G,⋅)(G,\cdot) be a finite group.

Definition A.
Let XX be a set. An action of the group GG on XX is any homomorphism φ\varphi from GG to S(X)S(X). We denote

g⋅x:=φ(g)(x)for (g,x)∈G×X.g\cdot x:=\varphi(g)(x) \quad\text{for } (g,x)\in G\times X.

If x∈Xx\in X, the stabilizer of xx is the set

Stab⁡(x)={g∈G∣g⋅x=x}.\operatorname{Stab}(x)=\{g\in G\mid g\cdot x=x\}.

It is straightforward to verify that this is a subgroup of GG. The action is said to be faithful if φ\varphi is injective, and transitive if for all x∈Xx\in X,

{g⋅x,  g∈G}=X.\{g\cdot x,\;g\in G\}=X.

Proposition A.
Suppose that GG acts on XX. Then for any g∈Gg\in G and x∈Xx\in X,

Stab⁡(g⋅x)=g Stab⁡(x) g−1.\operatorname{Stab}(g\cdot x)=g\,\operatorname{Stab}(x)\,g^{-1}.

Proof.
If h∈Stab⁡(g⋅x)h\in \operatorname{Stab}(g\cdot x), then

h⋅(g⋅x)=g⋅x⟺(g−1hg)⋅x=x⟺g−1hg∈Stab⁡(x),h\cdot (g\cdot x)=g\cdot x\quad\Longleftrightarrow\quad (g^{-1}hg)\cdot x=x\quad\Longleftrightarrow\quad g^{-1}hg\in \operatorname{Stab}(x),

i.e. h∈g Stab⁡(x) g−1h\in g\,\operatorname{Stab}(x)\,g^{-1}. □\square

Definition B.
Let (G,⋅)(G,\cdot) be a group.

  • For g∈Gg\in G, the map φg:x∈G↦gxg−1∈G\varphi_g: x\in G\mapsto gxg^{-1}\in G is an automorphism of the group, called the conjugation automorphism; and the map g↦φg∈Aut⁡(G)g\mapsto \varphi_g\in\operatorname{Aut}(G) defines an action of GG on itself.
  • Two elements x,y∈Gx,y\in G are said to be conjugate if there exists g∈Gg\in G such that x=φg(y)x=\varphi_g(y). This defines an equivalence relation on GG whose equivalence classes are called conjugacy classes. Similarly, one defines the conjugates of a subset of GG. If HH is a subgroup of GG, then for every g∈Gg\in G, φg(H)\varphi_g(H) is a subgroup of GG (being the image of a subgroup by a homomorphism) of cardinality ∣H∣|H| (since φg\varphi_g is injective).

Definition C.
Let HH be a subgroup of GG. We say that HH is normal if

∀ g∈G,  ∀ h∈H,ghg−1∈H.\forall\, g\in G,\;\forall\, h\in H,\quad ghg^{-1}\in H.

Definition D.
Let HH be a subgroup of GG. Two elements x,y∈Gx,y\in G are said to be congruent modulo HH if y−1x∈Hy^{-1}x\in H. This defines an equivalence relation on GG whose equivalence classes (the left cosets) are the sets

gH,g∈G.gH,\quad g\in G.

We denote

G/H={gH∣g∈G}.G/H=\{gH\mid g\in G\}.

Since for any g∈Gg\in G the map τg:h↦gh\tau_g: h\mapsto gh is injective, every coset has cardinality ∣H∣|H| and since their union is GG,

∣G/H∣=∣G∣∣H∣,|G/H|=\frac{|G|}{|H|},

which in particular shows that ∣H∣|H| divides ∣G∣|G| (this is Lagrange's Theorem).

Finally, we define the notion of a Hermitian space, which generalizes that of a Euclidean space:

Definition E.
Let VV be a C\mathbb{C}-vector space. A Hermitian inner product on VV is a function

⟨ ⋅ , ⋅ ⟩:V×V→C,\langle\,\cdot\,,\,\cdot\,\rangle: V\times V\to\mathbb{C},

which is linear in the second variable (i.e. for all x,y,z∈Vx,y,z\in V and λ∈C\lambda\in\mathbb{C}, ⟨x,y+λz⟩=⟨x,y⟩+λ⟨x,z⟩\langle x,y+\lambda z\rangle=\langle x,y\rangle+\lambda\langle x,z\rangle), Hermitian symmetric (i.e. ⟨x,y⟩=⟨y,x⟩‾\langle x,y\rangle=\overline{\langle y,x\rangle}), positive (i.e. ⟨x,x⟩∈R+\langle x,x\rangle\in\mathbb{R}_+ for all x∈Vx\in V), and definite (i.e. ⟨x,x⟩=0\langle x,x\rangle=0 if and only if x=0x=0). As in the Euclidean case, one defines the notion of orthogonality and orthonormal families.


Bibliography

  1. Gaëtan Chenevier
    Algebra I Course (Chapter 7, Linear Representations of Finite Groups)

  2. William Fulton and Joe Harris
    Representation Theory: A First Course.
    Springer, 2004.

  3. Gérard Rauch
    Finite Groups and Their Representations.
    Ellipses, 2000.
    ISBN: 978-2-7298-0180-9

  4. Jean-Pierre Serre
    Finite Groups: An Introduction.
    International Press, 2016.
    ISBN: 978-1-57146-327-2


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