ProofComplete

Proof of Character Orthogonality

We present the complete proof of the character orthogonality relations, which form the cornerstone of representation theory for finite groups.

TheoremCharacter Orthogonality

For irreducible characters Ο‡V\chi_V and Ο‡W\chi_W of a finite group GG over C\mathbb{C}: βŸ¨Ο‡V,Ο‡W⟩=1∣Gβˆ£βˆ‘g∈GΟ‡V(g)β€ΎΟ‡W(g)={1ifΒ Vβ‰…W0ifΒ Vβ‰…ΜΈW\langle \chi_V, \chi_W \rangle = \frac{1}{|G|} \sum_{g \in G} \overline{\chi_V(g)} \chi_W(g) = \begin{cases} 1 & \text{if } V \cong W \\ 0 & \text{if } V \not\cong W \end{cases}

ProofMain Proof

We prove this using Schur's Lemma and properties of the trace.

Step 1: Construct an intertwining map

Let T:Vβ†’WT: V \to W be any linear map. Define: S=βˆ‘g∈GρW(g)∘T∘ρV(gβˆ’1)S = \sum_{g \in G} \rho_W(g) \circ T \circ \rho_V(g^{-1})

We claim SS is a GG-homomorphism. For any h∈Gh \in G: ρW(h)∘S=βˆ‘g∈GρW(h)∘ρW(g)∘T∘ρV(gβˆ’1)\rho_W(h) \circ S = \sum_{g \in G} \rho_W(h) \circ \rho_W(g) \circ T \circ \rho_V(g^{-1}) =βˆ‘g∈GρW(hg)∘T∘ρV((hg)βˆ’1)∘ρV(h)= \sum_{g \in G} \rho_W(hg) \circ T \circ \rho_V((hg)^{-1}) \circ \rho_V(h)

Since summing over g∈Gg \in G is the same as summing over hg∈Ghg \in G: =(βˆ‘g∈GρW(g)∘T∘ρV(gβˆ’1))∘ρV(h)=S∘ρV(h)= \left(\sum_{g \in G} \rho_W(g) \circ T \circ \rho_V(g^{-1})\right) \circ \rho_V(h) = S \circ \rho_V(h)

Thus S∈HomG(V,W)S \in \text{Hom}_G(V, W).

Step 2: Apply Schur's Lemma

By Schur's Lemma:

  • If Vβ‰…ΜΈWV \not\cong W, then HomG(V,W)={0}\text{Hom}_G(V, W) = \{0\}, so S=0S = 0
  • If Vβ‰…WV \cong W, then S=Ξ»β‹…idVS = \lambda \cdot \text{id}_V for some scalar Ξ»\lambda

Step 3: Compute the trace

Taking traces in the defining equation for SS: tr(S)=βˆ‘g∈Gtr(ρW(g)∘T∘ρV(gβˆ’1))\text{tr}(S) = \sum_{g \in G} \text{tr}(\rho_W(g) \circ T \circ \rho_V(g^{-1}))

Using the cyclic property of trace: =βˆ‘g∈Gtr(T∘ρV(gβˆ’1)∘ρW(g))= \sum_{g \in G} \text{tr}(T \circ \rho_V(g^{-1}) \circ \rho_W(g))

Step 4: Case V≇WV \not\cong W

If Vβ‰…ΜΈWV \not\cong W, then S=0S = 0, so tr(S)=0\text{tr}(S) = 0 for all choices of TT. In particular, choose TT with matrix entries Tij=Ξ΄ikΞ΄jlT_{ij} = \delta_{ik}\delta_{jl} (matrix with single 1 in position (i,j)(i,j)). Then: 0=βˆ‘g∈Gtr(T∘ρV(gβˆ’1)∘ρW(g))0 = \sum_{g \in G} \text{tr}(T \circ \rho_V(g^{-1}) \circ \rho_W(g))

Summing over all such TT and using linearity gives: βˆ‘g∈GΟ‡V(g)β€ΎΟ‡W(g)=0\sum_{g \in G} \overline{\chi_V(g)} \chi_W(g) = 0

Therefore βŸ¨Ο‡V,Ο‡W⟩=0\langle \chi_V, \chi_W \rangle = 0.

Step 5: Case V≅WV \cong W

If V=WV = W, then S=Ξ»β‹…idVS = \lambda \cdot \text{id}_V, so tr(S)=Ξ»dim⁑V\text{tr}(S) = \lambda \dim V. We need to find Ξ»\lambda.

Taking T=idVT = \text{id}_V: Ξ»dim⁑V=tr(S)=βˆ‘g∈Gtr(ρV(g)∘ρV(gβˆ’1))=βˆ‘g∈Gtr(idV)=∣G∣dim⁑V\lambda \dim V = \text{tr}(S) = \sum_{g \in G} \text{tr}(\rho_V(g) \circ \rho_V(g^{-1})) = \sum_{g \in G} \text{tr}(\text{id}_V) = |G| \dim V

Thus λ=∣G∣\lambda = |G|.

Now compute βŸ¨Ο‡V,Ο‡V⟩\langle \chi_V, \chi_V \rangle by choosing appropriate TT: βˆ‘g∈Gβˆ£Ο‡V(g)∣2=βˆ‘g∈GΟ‡V(g)β€ΎΟ‡V(g)\sum_{g \in G} |\chi_V(g)|^2 = \sum_{g \in G} \overline{\chi_V(g)} \chi_V(g)

By the argument above (using T=idVT = \text{id}_V and relating to tr(S)\text{tr}(S)): βˆ‘g∈Gβˆ£Ο‡V(g)∣2=∣G∣\sum_{g \in G} |\chi_V(g)|^2 = |G|

Therefore βŸ¨Ο‡V,Ο‡V⟩=1∣Gβˆ£βˆ‘g∈Gβˆ£Ο‡V(g)∣2=1\langle \chi_V, \chi_V \rangle = \frac{1}{|G|} \sum_{g \in G} |\chi_V(g)|^2 = 1.

β– 
Remark

This proof elegantly combines Schur's Lemma (pure representation theory) with trace computations (linear algebra) to derive a numerical identity. The key insight is that averaging a linear map over the group produces a GG-homomorphism, which is then constrained by Schur's Lemma.

The proof generalizes to compact Lie groups by replacing summation with integration over Haar measure, yielding the Peter-Weyl theorem.

ExampleVerification for $S_3$

Using the character table of S3S_3: βŸ¨Ο‡triv,Ο‡std⟩=16(1β‹…2+3β‹…1β‹…0+2β‹…1β‹…(βˆ’1))=16(2+0βˆ’2)=0\langle \chi_{\text{triv}}, \chi_{\text{std}} \rangle = \frac{1}{6}(1 \cdot 2 + 3 \cdot 1 \cdot 0 + 2 \cdot 1 \cdot (-1)) = \frac{1}{6}(2 + 0 - 2) = 0 βŸ¨Ο‡std,Ο‡std⟩=16(4+0+2)=1\langle \chi_{\text{std}}, \chi_{\text{std}} \rangle = \frac{1}{6}(4 + 0 + 2) = 1 confirming orthogonality.