I am currently studying the book Lie Algebras in Particle Physics by Howard Georgi (2nd edition) and I couldn't understand this part:
A representation is completely reducible if it is equivalent to a representation whose matrix elements have the following form: $$\begin{bmatrix}D_1(g) & 0 & 0\ ... \\0&D_2(g) &0\ ... \\ ...\ & ...\ & ... \end{bmatrix}$$ where $D_j(g)$ is irreducible for all $j$. This is called block diagonal form.
Notation: $g$ refers to an element of a group $G$ and $D$ is a representation.
What I don't quite get is: Those diagonal elements are just numbers aren't they? Then what's with calling them irreducible representations? Going further, the author says:
A representation in block diagonal form is said to be the direct sum of the subrepresentations, $D_j$s
I am a beginner so excuse me if this is trivial. Why exactly did he say that those matrix elements are representations themselves? What am I missing?