Spatial isomorphism between type I factors

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I'm reading a paper from Christopher J. Fewster about split property, and I'm trying to catch one of his assertions.

He asserts that every type I factor $M$ (a concrete von Neumann algebra over $\mathcal{H}$) is spatially isomorphic with $B(\mathcal{K})\otimes \mathbb{1}_{\mathcal{K'}}$. Implemented by a isomorphism $U:\mathcal{H}\to \mathcal{K}\otimes \mathcal{K}'$ such that $UMU^{-1}=B(\mathcal{K})\otimes \mathbb{1}_{\mathcal{K'}}$.

Basically I don't underestand who are $\mathcal{K}$, $\mathcal{K}'$ and what is exactly the isomorphism $U$.

In spite of He give us a reference, I failed trying to understand it because it wasn't the explicit construction there.

Many thanks in advance!

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We are assuming that $M$ is not degenerate (i.e., it has the same unit as $B(H)$). Because $M$ is type I, it the sot-closed-span of a family $\{E_{kj}\}_{kj\in S}$ of matrix units. In the decomposition you want, $\dim K=|S|$, and $\dim K'=\operatorname{Tr}(E_{11})$. Let $Z$ be any index set with $|Z|=\operatorname{Tr}(E_{11})$.

Explicitly, form an orthonormal basis $\{e_{k\ell}\}_{k,\in S,\ \ell\in Z}$ for $H$, where $E_{kk}H=\operatorname{span}\{e_{k\ell}\}_{\ell\in Z}$, and $E_{kj}e_{j\ell}=e_{k\ell}$. Such a thing exists because $\operatorname{Tr}(E_{kk})=\operatorname{Tr}(E_{11})$ for all $k$ and $\sum_kE_{kk}=1$. Let $K,K'$ be Hilbert spaces with $\dim K=|S|$, $\dim K'=|Z|$ and orthonormal bases $\{e_{k}\}_{k\in S}$, $\{f_\ell\}_{\ell\in Z}$ respectively. Define $U:H\to K\otimes K'$ by $$ Ue_{k\ell}=e_k\otimes f_\ell $$ and extend by linearity. Because $U$ maps an orthonormal basis to an orthonormal basis, it is a unitary.

Let $\{E_{kj}'\}$ be matrix units for $K$, associated with the basis $\{e_k\}$. Then \begin{align} UE_{kj}e_{h\ell}&=\delta_{jh}Ue_{k\ell}=\delta_{jh}\,(e_k\otimes f_\ell), \end{align} and $$ (E_{kj}'\otimes 1_{K'})Ue_{h\ell} =(E_{kj}'\otimes 1_{K'})(e_h\otimes f_\ell) =\delta_{jk}\,(e_k\otimes f_\ell). $$ As we get the equality for all elements in the basis, $UE_{kj}=(E'_{kj}\otimes 1_{K'})U$. Since $U$ is a unitary, $UE_{kj}U^*=E'_{kj}\otimes 1_{K'}$. As both on $B(H)$ and $B(K)$ the span of the matrix units is sot-dense, this conjugation by $U$ extends to a $*$-isomorphism, and so $$ UMU^*=B(K)\otimes 1_{K'}. $$ If anything of the above is hard to follow, consider the case where $$ M=\left\{\begin{bmatrix} a&0&0&b&0&0\\ 0&a&0&0&b&0\\ 0&0&a&0&0&b\\ c&0&0&d&0&0\\ 0&c&0&0&d&0\\ 0&0&c&0&0&d\\ \end{bmatrix}:\ a,b,c,d\in\mathbb C\right\}. $$