decomposition of self-adjoint elements in positive and negative parts
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decomposition
Every real valued function admits a well-known decomposition into its and parts: . There is an analogous result for self-adjoint elements in a -algebra (http://planetmath.org/CAlgebra) that we will now describe.
Theorem - Let be a -algebra and a self-adjoint element. Then there are unique positive elements and in such that:
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Both and belong to -subalgebra generated by .
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Remark - As a particular case, the result provides a decomposition of each self-adjoint operator on a Hilbert space as a difference of two positive operators such that and , where and denote, respectively, the range and kernel of an operator
.
Proof:
Let us some notation first:
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denotes the spectrum of .
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denotes the -subalgebra generated by .
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denotes the algebra of continuous functions
in that vanish at infinity.
Let be the functions defined by
Since is , , so the above functions are well defined. It is clear that
(1) |
The continuous functional calculus gives an isomorphism such that the element corresponds to the function . Let and be the elements corresponding to and respectively. From the made in (1) it is now clear that
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and are both positive elements.
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Both and belong to .
From the fact the every -isomorphism is isometric (see this entry (http://planetmath.org/HomomorphismsOfCAlgebrasAreContinuous)) and it follows that .
The uniqueness of the decomposition follows from the uniqueness of the decomposition of real valued functions in its positive and negative parts (with ).