The sum of two extension is defined in the following way:
Let $\mathcal{B}$ and $\mathcal{A}$ be two separable C*-algebras with $\mathcal{B}$ stable and $\phi,\psi: \mathcal{A} \rightarrow \mathcal{M(B)/B}$ be two extensions of $\mathcal{B}$ by $\mathcal{A}$. Then the sum of extension is defined in the following way: $$(\phi \oplus \psi)(a)=\pi(S)\phi(a)\pi(S^*)+\pi(T)\psi(a)\pi(T^*)$$ where $S,T \in \mathcal{M(B)}$ are isometries such that $SS^*+TT^*=1_{\mathcal{M(B)}}$.
I do not follow the motivation why we define the sum in this way and what is the guarantee that we find two such isometries $S$ and $T$ such that $SS^*+TT^*=1_{\mathcal{M(B)}}$.
Can you refer me some notes or papers where I can find the details of this BDF sum?
Also I do not get the idea why we define the BDF equivalance of extensions as follows:
Two extensions $\phi$ and $\psi$ are equivalent if there exists $\rho,\sigma: \mathcal{A} \rightarrow \mathcal{M(B)/B}$ trivial extensions such that $$\phi \oplus \rho \sim_u \psi \oplus \sigma$$
Any reference of notes and paper will be very helpful. Thanks in advance.
In "Elements of KK-theory" by Jensen and Thomsen, the multiplier algebra is thought of as the space of adjointable operators on $B$ as a right Hilbert $B$-module. In the first couple of sections, it is shown that $\mathcal{L}_B(\mathcal{H}_B) \simeq \mathcal{M}(\mathbb{K} \otimes B)$, which is in turn isomorphic to $\mathcal{M}(B)$ by stability. $\mathcal{H}_B$ is a lot like a countable infinite-dimensional Hilbert space, so proceed how you would in $\mathcal{B}(H)$ to get two isometries $S,T$ such that $SS^* + TT^* = 1$.
– PStheman Nov 12 '19 at 22:47