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decomposition of self-adjoint elements in positive and negative parts (Theorem)

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.

$\,$

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 $a$ .
  • $\|a\| = \max\{\|a_+\|, \|a_-\|\}$

$\,$

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.

$\,$

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

$\displaystyle f(t):=t \qquad\qquad f_+(t) := \begin{cases}t, & $if$\;\; t \geq ... ...(t):= \begin{cases}0, & $if$\;\; t \geq 0\\ -t, & $if$\;\; t \leq 0 \end{cases}$    

Since $a$ is self-adjoint, $\sigma(a) \subseteq \mathbb{R}$ , so the above functions are well defined. It is clear that
$\displaystyle f = f_+ - f_- \;\;\;$and$\displaystyle \;\;\; f_+f_-=f_-f_+=0 \;\;\;$and$\displaystyle \;\;\; f_+, f_- \;$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: $C^*$-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 MSC46L05 (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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