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decomposition of self-adjoint elements in positive and negative parts
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(Theorem)
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Every real valued function $f$ admits a well-known decomposition into its positive and negative parts: $f = f_+ - f_-$ . There is an analogous result for self-adjoint elements in a $C^*$ -algebra that we will now describe.
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Theorem - Let $\mathcal{A}$ be a $C^*$ -algebra and $a \in \mathcal{A}$ a self-adjoint element. Then there are unique positive elements $a_+$ and $a_-$ in $\mathcal{A}$ such that:
- $a= a_+ - a_-$
- $a_+a_- = a_-a_+ = 0$
- Both $a_+$ and $a_-$ belong to $C^*$ -subalgebra generated by $a$ .
- $\|a\| = \max\{\|a_+\|, \|a_-\|\}$
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Remark - As a particular case, the result provides a decomposition of each self-adjoint operator $T$ on a Hilbert space as a difference of two positive operators $T=T_+ - T_-$ such that $\mathrm{Ran}\; T_- \subseteq \mathrm{Ker}\; T_+$ and $\mathrm{Ran}\; T_+ \subseteq \mathrm{Ker}\; T_-$ , where $\mathrm{Ran}\;$ and $\mathrm{Ker}\;$ denote, respectively, the range and kernel of an operator.
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Proof:
Let us fix some notation first:
Let $f, f_+, f_- \in C_0\big(\sigma(a)\setminus \{0\}\big)$ be the functions defined by
Since $a$ is self-adjoint, $\sigma(a) \subseteq \mathbb{R}$ , so the above functions are well defined. It is clear that
and and are both positive |
(1) |
The continuous functional calculus gives an isomorphism $C^*[a] \cong C_0\big(\sigma(a)\setminus \{0\}\big)$ such that the element $a$ corresponds to the function $f$ . Let $a_+$ and $a_-$ be the elements corresponding to $f_+$ and $f_-$ respectively. From the observations made in (1) it is now clear that
- $a_+$ and $a_-$ are both positive elements.
- $a = a_+ - a_-$
- $a_+a_- = a_-a_+ = 0$
- Both $a_+$ and $a_-$ belong to $C^*[a]$ .
From the fact the every $C^*$ -isomorphism is isometric (see this entry) and $\|f\| = \max\{\|f_+\|, \|f_-\|\}$ it follows that $\|a\| = \max\{\|a_+\|, \|a_-\|\}$ .
The uniqueness of the decomposition follows from the uniqueness of the decomposition of real valued functions in its positive and negative parts $f = f_+-f_-$ (with $f_+f_- = 0$ ). $\square$
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See Also: -algebra
| Keywords: |
self-adjoint element decomposition |
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Cross-references: negative, isometric, isomorphism, continuous functional calculus, clear, well defined, vanish at infinity, continuous functions, algebra, spectrum, proof, operator, kernel, range, positive operators, difference, Hilbert space, self-adjoint operator, generated by, positive elements, theorem, self-adjoint elements, function, real
This is version 9 of decomposition of self-adjoint elements in positive and negative parts, born on 2008-02-26, modified 2008-11-08.
Object id is 10341, canonical name is DecompositionOfSelfAdjointElementsInPositiveAndNegativeParts.
Accessed 635 times total.
Classification:
| AMS MSC: | 46L05 (Functional analysis :: Selfadjoint operator algebras :: General theory of $C^*$-algebras) | | | 47A60 (Operator theory :: General theory of linear operators :: Functional calculus) | | | 47B25 (Operator theory :: Special classes of linear operators :: Symmetric and selfadjoint operators ) | | | 47C15 (Operator theory :: Individual linear operators as elements of algebraic systems :: Operators in $C^*$- or von Neumann algebras) |
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Pending Errata and Addenda
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