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Positive element

In mathematics, an element of a *-algebra is called positive if it is the sum of elements of the form a^{*}a.

01Definition

Let {\mathcal {A}} be a *-algebra. An element a\in {\mathcal {A}} is called positive if there are finitely many elements a_{k}\in {\mathcal {A}}\;(k=1,2,\ldots ,n), so that {\textstyle a=\sum _{k=1}^{n}a_{k}^{*}a_{k} holds. This is also denoted by a\geq 0.

The set of positive elements is denoted by {\mathcal {A}}_{+}.

A special case from particular importance is the case where {\mathcal {A}} is a complete normed *-algebra, that satisfies the C*-identity (\left\|a^{*}a\right\|=\left\|a\right\|^{2}\ \forall a\in {\mathcal {A}}), which is called a C*-algebra.

02Examples

  • The unit element e of an unital *-algebra is positive.
  • For each element a\in {\mathcal {A}}, the elements a^{*}a and aa^{*} are positive by definition.

In case {\mathcal {A}} is a C*-algebra, the following holds:

03Criteria

Let {\mathcal {A}} be a C*-algebra and a\in {\mathcal {A}}. Then the following are equivalent:

  • For the spectrum \sigma (a)\subseteq [0,\infty ) holds and a is a normal element.
  • There exists an element b\in {\mathcal {A}}, such that a=bb^{*}.
  • There exists a (unique) self-adjoint element c\in {\mathcal {A}}_{sa} such that a=c^{2}.

If {\mathcal {A}} is a unital *-algebra with unit element e, then in addition the following statements are equivalent:

  • \left\|te-a\right\|\leq t for every t\geq \left\|a\right\| and a is a self-adjoint element.
  • \left\|te-a\right\|\leq t for some t\geq \left\|a\right\| and a is a self-adjoint element.

04Properties

In *-algebras

Let {\mathcal {A}} be a *-algebra. Then:

  • If a\in {\mathcal {A}}_{+} is a positive element, then a is self-adjoint.
  • The set of positive elements {\mathcal {A}}_{+} is a convex cone in the real vector space of the self-adjoint elements {\mathcal {A}}_{sa}. This means that \alpha a,a+b\in {\mathcal {A}}_{+} holds for all a,b\in {\mathcal {A}} and \alpha \in [0,\infty ).
  • If a\in {\mathcal {A}}_{+} is a positive element, then b^{*}ab is also positive for every element b\in {\mathcal {A}}.
  • For the linear span of {\mathcal {A}}_{+} the following holds: \langle {\mathcal {A}}_{+}\rangle ={\mathcal {A}}^{2} and {\mathcal {A}}_{+}-{\mathcal {A}}_{+}={\mathcal {A}}_{sa}\cap {\mathcal {A}}^{2}.

In C*-algebras

Let {\mathcal {A}} be a C*-algebra. Then:

  • Using the continuous functional calculus, for every a\in {\mathcal {A}}_{+} and n\in \mathbb {N} there is a uniquely determined b\in {\mathcal {A}}_{+} that satisfies b^{n}=a, i.e. a unique n-th root. In particular, a square root exists for every positive element. Since for every b\in {\mathcal {A}} the element b^{*}b is positive, this allows the definition of a unique absolute value: {\textstyle |b|=(b^{*}b)^{\frac {1}{2}}.
  • For every real number \alpha \geq 0 there is a positive element a^{\alpha }\in {\mathcal {A}}_{+} for which a^{\alpha }a^{\beta }=a^{\alpha +\beta } holds for all \beta \in [0,\infty ). The mapping \alpha \mapsto a^{\alpha } is continuous. Negative values for \alpha are also possible for invertible elements a.
  • Products of positive commutative elements are also positive. So if ab=ba holds for positive a,b\in {\mathcal {A}}_{+}, then ab\in {\mathcal {A}}_{+}.
  • Each element a\in {\mathcal {A}} can be uniquely represented as a linear combination of four positive elements. To do this, a is first decomposed into the self-adjoint real and imaginary parts and these are then decomposed into positive and negative parts using the continuous functional calculus. For it holds that {\mathcal {A}}_{sa}={\mathcal {A}}_{+}-{\mathcal {A}}_{+}, since {\mathcal {A}}^{2}={\mathcal {A}}.
  • If both a and -a are positive a=0 holds.
  • If {\mathcal {B}} is a C*-subalgebra of {\mathcal {A}}, then {\mathcal {B}}_{+}={\mathcal {B}}\cap {\mathcal {A}}_{+}.
  • If {\mathcal {B}} is another C*-algebra and \Phi is a *-homomorphism from {\mathcal {A}} to {\mathcal {B}}, then \Phi ({\mathcal {A}}_{+})=\Phi ({\mathcal {A}})\cap {\mathcal {B}}_{+} holds.
  • If a,b\in {\mathcal {A}}_{+} are positive elements for which ab=0, they commutate and \left\|a+b\right\|=\max(\left\|a\right\|,\left\|b\right\|) holds. Such elements are called orthogonal and one writes a\bot b.

05Partial order

Let {\mathcal {A}} be a *-algebra. The property of being a positive element defines a translation invariant partial order on the set of self-adjoint elements {\mathcal {A}}_{sa}. If b-a\in {\mathcal {A}}_{+} holds for a,b\in {\mathcal {A}}, one writes a\leq b or b\geq a.

This partial order fulfills the properties ta\leq tb and a+c\leq b+c for all a,b,c\in {\mathcal {A}}_{sa} with a\leq b and t\in [0,\infty ).

If {\mathcal {A}} is a C*-algebra, the partial order also has the following properties for a,b\in {\mathcal {A}}:

  • If a\leq b holds, then c^{*}ac\leq c^{*}bc is true for every c\in {\mathcal {A}}. For every c\in {\mathcal {A}}_{+} that commutes with a and b even ac\leq bc holds.
  • If -b\leq a\leq b holds, then \left\|a\right\|\leq \left\|b\right\|.
  • If 0\leq a\leq b holds, then {\textstyle a^{\alpha }\leq b^{\alpha } holds for all real numbers 0<\alpha \leq 1.
  • If a is invertible and 0\leq a\leq b holds, then b is invertible and for the inverses b^{-1}\leq a^{-1} holds.
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Sources and credits

This article is adapted from the Wikipedia article Positive element, written by its contributors and licensed under CC BY-SA 4.0. Fathomly has changed the layout, removed citation markers, navigation and maintenance notices, and adjusted punctuation. This adapted version is shared under the same license. For references, see the original article.

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