Here is a quotation in a book "C*-algebrass and Finite-Dimensional Approximations" by Nate and Taka (P122).
Let $A$ be a C*-algebra, $\Gamma$ be a discrete group and the $\alpha$ is an action of $\Gamma$ on $A$. If $F\subset \Gamma$ is a finite set, define $\psi: A\otimes M_{F}(\mathbb{C})\rightarrow C_{c}(\Gamma, A)$ by $$\psi(a\otimes e_{p, q})=\frac{1}{|F|}\alpha_{p}(a)\lambda_{pq^{-1}}.$$
then $\psi$ is a contractive completely positive map.
In fact, in order to prove completely positive map, it suffices to prove that $\psi$ is positive since Exercise 4.1.3 provides a natural commutative diagram:
$$M_{n}(\mathbb{C})\otimes(A\otimes M_{F}(\mathbb{C}))\cong (M_{n}(\mathbb{C})\otimes A)\otimes M_{F}(\mathbb{C})$$
$$~~~~\downarrow~~~~~~~~~~~~~~~~~~~~~~~~~~~~\downarrow$$
$$M_{n}(\mathbb{C})\otimes(A\rtimes_{\alpha,r}\Gamma)\cong M_{n}(\mathbb{C})\otimes(A\rtimes_{\tau\otimes\alpha,r}\Gamma)$$
Exercise 4.1.3. Let $A$ and $B$ be two C*-algebras and $\Gamma$ be a discrete group. If $\alpha:\Gamma\rightarrow \mathrm{Aut}(A)$ is an action and $\tau\otimes\alpha:\Gamma\rightarrow Aut(B\otimes A)$ is defined by $(\tau\otimes\alpha)_{g}=\mathrm{id}_{B}\otimes\alpha_{g}$, then $$(B\otimes A)\rtimes_{\tau\otimes\alpha, r}\Gamma\cong B\otimes(A\rtimes_{\alpha, r}\Gamma).$$
My question:
How to verify $\psi$ is contractive?
How to use the commutative diagram to "reduce" the completely positive to positive?
1: On a quick look, I don't immediately see how to show that $\psi$ is contractive in general. But note that when $A$ is unital so is $\psi$, which together with positivity makes it contractive. I think this idea can be extended to the non-unital case.
2: When you prove that $\psi$ is positive, you don't need to use that $A$ is $A$, just that it is a C$^*$-algebra. In particular the same proof works for $M_n(\mathbb C)\otimes A$. This gives you the down arrow on the right of the diagram as a positive map. The commutativity of the diagram then tells you that the left down arrow is a positive map, and this is $\psi^{(n)}$. The same argument applies to contractivity.