In this post, I mainly focus on introducing Gelfand pairs of finite groups.
Representations of finite groups
Let’s recall some concepts. Let \(G\) be a finite group. A (complex) representation of \(G\) is a pair \((\rho, V)\) where \(V\) is a vector space over \(\C\) and \(\rho: G \to GL(V)\) is a group homomorphism. Let \((\rho_1, V_1)\) and \((\rho_2, V_2)\) be representations of \(G\), a \(G\)-morphism, or simply a morphism, between these two representations is a linear map \(\varphi: V_1 \to V_2\) such that for any \(g \in G\) and \(v \in V_1\),
\[\varphi(\rho_1(g)v) = \rho_2(g)\varphi(v).\]
Then \(\mathrm{Hom}_G(\rho_1, \rho_2)\), the set of morphisms between \(\rho_1\) and \(\rho_2\), is a vector space over \(\C\). A representation \((\rho, V)\) is irreducible, if there is no proper subspace \(W \subset V\), such that \(\rho(g)w \in W\) for any \(g \in G\) and \(w \in W\). Between irreducible representations, we have Schur’s lemma.
Theorem 1 (Schur’s lemma).
Let
\(\rho_1\) and
\(\rho_2\) be irreducible representations of
\(G\). Then
\[\begin{equation*}
\mathrm{Hom}_G(\rho_1, \rho_2) \cong \left\{
\begin{array}{ll}
\C, & \text{ if } \rho_1 \cong \rho_2; \\
0, & \text{ otherwise.}
\end{array}
\right.
\end{equation*}\]
It’s well known that \(G\) is semisimple, i.e., any representation of \(G\) decomposes into a direct sum of irreducible representations. A representation \((\rho, V)\) of \(G\) is called multiplicity free, if any irreducible representation appearing in the decomposition of \((\rho, V)\) appears exactly once, up to isomorphism.
Let \(H\) be a subgroup of \(G\). If \((\rho, V)\) is a representation of \(G\), we can certainly restrict the group homomorphism \(\rho: G \to GL(V)\) to \(H\) so that we can regard \((\rho, V)\) as a representation of \(H\). This is called the restriction of representations from \(G\) to \(H\), and the restricted representation of \(\rho\) will be denoted as \(r^G_H(\rho)\). Conversely, if \((\pi, W)\) is a representation of \(H\), we can build a representation \((\rho, V)\) of \(G\) out of \(\pi\), which is the induced representation, as follow.