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A projection is a bounded self-adjoint idempotent operator acting on . We denote by (or for brevity if there is no ambiguity) the set of all projections in . For define
This relation is a partial order on . It is known that is a complete lattice with respect to [see ?]. Since projections are selfadjoint, for any two projections. Hence the dual relation defined by
for any two projection and , coincides with the relation defined above.
If is a projection then the image of :
is a closed subspace of uniquely determined by . Subspaces of arising in this way are called subspaces belonging to . Let [or simply for brevity] denote the set of all subspaces belonging to . is partially ordered set with respect to inclusion. Furthermore, this gives a mapping
which is an order-isomorphism. For , let , denote the unique projection with . Then the map is also an order-isomorphism of onto and is the inverse of .
Similarly to each we can associate a closed subspace
is an order-reversing dual isomorphism of onto . Furthermore, we have
In the following we use the notations and terminology from Nambooripad [1979] associated with biordered sets. In particular, the set of all idempotents of a semigroup is a biordered set with respect to the partial binary operation on induced from ([see Nambooripad, 1979, Theorem 1]). Therefore given a von Neumann algebra , the set of all idempotents in is the biordered set of idempotents of the multiplicative semigroup of . It is well known that a von Neumann algebra is uniquely determined by the set projections of [see ?]. Since , it follows that the algebra is uniquely determined by the biordetred set . Hence we shall refer to as the biordered set of . We thus infer that for every von Neumann algebra , is a nonempty and non-trivial biordered set.
Let . Since is a continuous idempotent,
are closed and complementary subspaces in . Therefore is a complementary pair of subspaces in associated with the idempotent ; for brevity, we will denote by a complementary pair of subspaces in .
Proposition 8.1. Every idempotent in is associated with a pair of complementary subspaces in . Conversely, let be any complementary pair of subspaces in and let and are projections determined by the subspaces and respectively. Then
Therefore the map is a bijection of onto the set of all complementary pairs of subspaces in .
Proof. The remarks preceding the statement shows that every idempotent determines a unique pair of complementary subspaces in . Conversely, let be any pair of complementary subspaces in . Since is a bijection there exist unique and in such that and . Then is a projection such that and . Then and are complements of . It follows that is a linear homeomorphism of onto . Hence
Now is a projection such that . Also by Equation (1) and (2) . Since the map is an order-isomorphism we have . Similarly . Clearly both and are idempotents. Also by equation (1) and since is a linear homeomorphism of onto , . Since and are projections in , is an idempotent in . Thus the idempotent satisfies all the requirements. Since and are projections uniquely determined by and respectively the idempotent is uniquely determined by the pair . It follows that the assignments is a bijection.
The result above shows that we may identify idempotents in with the corresponding complementary pair of subspaces in by the correspondence so that will also denote the set of all complementary pairs of subspaces in . Here it will be useful to determine explicitly the biorder structure on in terms of complementary pairs of subspaces in . Recall that basis of the structure of a biordered set on a set consists of two quasiorder relations on denoted by and respectively and a partial binary operation determined by these relations [see Chapter 3 in E. Krishnan, 2000].
Let , . Then for each , by Proposition 8.1, there exist complementary pairs of subspaces with
Given idempotents , it follows that [see for example Clifford and Preston, 1961, § 2.2 Exercise 6] that if and only if . In this case we can show that the basic product
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