Let $k$ be an algebraically closed field of characteristic $0$ and $G$ a finite group. The representation theory of $G$ is essentially the same the as the module theory over the (non commutative) algebra $k[G]$. Now, it is a well known fact that there is an isomorphism as algebras: $$k[G] \to \bigoplus_i M_{n_i}(k)$$ where $i$ runs over the irreducible representations of $G$ and $n_i$ is the dimension of the $i$-th representation, denoted by $V_i$. The problem is, I know two distinct ways of defining the above map. I suspect they are the same thing but can't show it.
The First Way: Consider $R = k[G]$ as a simple module over $k[G]$. There is an isomorphism, as modules: $$k[G] \cong \bigoplus_i V_i^{n_i}.$$ Applying the function $End_{k[G]}( -)$ on both sides, we obtain and isomorphism: $$\mu: k[G]^{opp} \to \bigoplus_i M_{n_i}(k).$$ On the right, the element $g$ corresponds to the $G-$ endomorphism of $R$ that sends $a \to ag$ for $a \in R$. On the right, the isomorphism with the matrix algebras is because of Schur's lemma and an element in $M_{n_i}(k)$ acts on $V_i^{n_i}$ by treating each $V_i$ as a one dimensional vector space essentially.
The second way: Now, for each $V_i$, the representation gives us a map $\rho_i: G \to GL_{n_i}(k)$ where $GL_n(k)$ is the invertible linear maps on $V_i$ (just one copy this time!). We can extend linearly to $\rho_i: k[G] \to M_{n_i}(k)$ and put everything together to get a map: $$\rho: k[G] \to \bigoplus_i M_{n_i}(k).$$
Now, it isn't clear to me at all that these two maps $\mu, \rho$ are the same thing. In particular, we need to show:
Fix a module isomorphism $\theta: kG \to \bigoplus_i V_i^{n_i}$. Then, define the map $R_h$ on $kG$ that sends $g \to gh$. This will translate into an endomorphism on the $V_i^{n_i}$ and since it is equivariant, we can represent it by an element in $\bigoplus_i M_{n_i}(V_i)$ where in the $i-th factor$, the entries of the matrix correspond to the trace of $R_h$ restricted to various factors. The question is whether on the $i-th$ factor, the matrix thus defined is equal to $\rho_i(h)$, the matrix defining the representation
For one, there is the small detail that $\mu$ has domain $k[G]^{opp}$ while $\rho$ has domain $k[G]$ but we can consider $\mu^{opp}$ instead since matrix algebras are self dual.
Second, there is the bigger issue that the two matrix algebras on the right act on different things in different ways. The first matrix algebra acts on $V_i^{n_i}$ by $G$-linear endomorphisms. The second matrix algebra acts on $V_i$ by simply linear endomorphisms.
Third: If we remove condition that $k$ be algebraically closed, then in the case of $\mu$, the fields $k$ are replaced by appropriate division algebras (and the number of direct summands = number of representations goes down).
However, in the case of $\rho$, the number of direct summands goes down as before but I don't think the field $k$ gets replaced by a division algebra.
Given this three points, I am doubtful wether $\mu$ and $\rho$ are really the same but it somehow seems even more improbable that we get distinct maps like this. What is going on here?
Of course, there is quite a bit of choice involved in defining these maps so the best we can hope for is that $\rho,\mu$ are equivalent, not equal on the nose.
Let $R$ be the regular representation, $h$ an element of $G$, $R_h$ the $G$-equivariant endomorphism or $k[G]$ that sends $g \to gh$. Let $\theta: kG \to \bigoplus_i V_i^{n_i}$ be an isomorphism and fix $i$.
Also, let $\pi: k[G] \to V_i^{n_i}$ be the projection map induced by $\theta$. Through $\theta$, $R_h$ acts on the $V_i^{n_i}$ since it is $G$-equivariant. Moreover, the action is by a scalar on each component by Schur's lemma.
That is, we can represent $R_h$ by a scalar $A = [a_{ij}]$ so that for a vector $v = (v_1,v_2,\dots,v_{n_i}) \in V_i^{n_i}$, $R_h$ sends it to $Av$. Explicitly, $v_l \to \sum_k a_{lk}v_k$.
On the other hand, consider the image of the identity element $\pi(e)$ in $V_i^{n_i}$. Let $\pi(e) = (v_1,v_2,\dots,v_n)$. Since $\pi$ is a surjection and $G\pi(e)$ generates all of $V_i^{n_i}$, the $v_1,\dots, v_n$ are linearly independent in $V_i$ and hence form a basis for it.
Moreover, $\pi(R_h(e)) = \pi(h) = h\pi(e) = (hv_1,hv_2,\dots,hv_n)$ but this is also equal to the image of $(v_1,\dots,v_n)$ under $R_h$ (or $A$). Let $h = [h_ij]$ as a matrix on $V_i$ in the basis $v_1,\dots,v_{n_i}$.
Therefore, $\sum_kh_{lk}v_k = hv_{l} = \sum_k a_{lk}v_k$ and since the $v_k$ are linearly independent, this implies that $h_{lk} = a_{lk}$.
That is, $R_h$ acts on $V_{n_i}$ by the matrix given by $h$.