positive element
In mathematics, an element of a *-algebra is called positive if it is the sum of elements of the form {{nowrap|.{{sfn|Palmer|2001|p=798}}}}
Definition
Let be a *-algebra. An element is called positive if there are finitely many elements , so that {{nowrap|holds.{{sfn|Palmer|2001|p=798}}}} This is also denoted by {{nowrap|.{{sfn|Blackadar|2006|p=63}}}}
The set of positive elements is denoted by {{nowrap|.}}
A special case from particular importance is the case where is a complete normed *-algebra, that satisfies the C*-identity (), which is called a C*-algebra.
Examples
- The unit element of an unital *-algebra is positive.
- For each element , the elements and are positive by {{nowrap|definition.{{sfn|Palmer|2001|p=798}}}}
In case is a C*-algebra, the following holds:
- Let be a normal element, then for every positive function which is continuous on the spectrum of the continuous functional calculus defines a positive element {{nowrap|.{{sfn|Kadison|Ringrose|1983|p=271}}}}
- Every projection, i.e. every element for which holds, is positive. For the spectrum of such an idempotent element, holds, as can be seen from the continuous functional {{nowrap|calculus.{{sfn|Kadison|Ringrose|1983|p=271}}}}
Criteria
Let be a C*-algebra and {{nowrap|.}} Then the following are equivalent:{{sfn|Kadison|Ringrose|1983|pages=247-248}}
- For the spectrum holds and is a normal element.
- There exists an element , such that {{nowrap|.}}
- There exists a (unique) self-adjoint element such that {{nowrap|.}}
If is a unital *-algebra with unit element , then in addition the following statements are {{nowrap|equivalent:{{sfn|Kadison|Ringrose|1983|p=245}}}}
- for every and is a self-adjoint element.
- for some and is a self-adjoint element.
Properties
= In *-algebras =
Let be a *-algebra. Then:
- If is a positive element, then is self-adjoint.{{sfn|Palmer|2001|p=800}}
- The set of positive elements is a convex cone in the real vector space of the self-adjoint elements {{nowrap|.}} This means that holds for all and {{nowrap|.{{sfn|Palmer|2001|p=800}}}}
- If is a positive element, then is also positive for every element {{nowrap|.{{sfn|Blackadar|2006|p=64}}}}
- For the linear span of the following holds: and {{nowrap|.{{sfn|Palmer|2001|p=802}}}}
= In C*-algebras =
Let be a C*-algebra. Then:
- Using the continuous functional calculus, for every and there is a uniquely determined that satisfies , i.e. a unique -th root. In particular, a square root exists for every positive element. Since for every the element is positive, this allows the definition of a unique absolute value: {{nowrap|.{{sfn|Blackadar|2006|pages=63-65}}}}
- For every real number there is a positive element for which holds for all {{nowrap|.}} The mapping is continuous. Negative values for are also possible for invertible elements {{nowrap|.{{sfn|Blackadar|2006|p=64}}}}
- Products of commutative positive elements are also positive. So if holds for positive , then {{nowrap|.{{sfn|Kadison|Ringrose|1983|p=245}}}}
- Each element can be uniquely represented as a linear combination of four positive elements. To do this, 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 {{nowrap|calculus.{{sfn|Kadison|Ringrose|1983|p=247}}}} For it holds that , since {{nowrap|.{{sfn|Palmer|2001|p=802}}}}
- If both and are positive {{nowrap|holds.{{sfn|Kadison|Ringrose|1983|p=245}}}}
- If is a C*-subalgebra of , then {{nowrap|.{{sfn|Kadison|Ringrose|1983|p=245}}}}
- If is another C*-algebra and is a *-homomorphism from to , then {{nowrap|holds.{{sfn|Dixmier|1977|p=18}}}}
- If are positive elements for which , they commutate and holds. Such elements are called orthogonal and one writes {{nowrap|.{{sfn|Blackadar|2006|p=67}}}}
Partial order
Let be a *-algebra. The property of being a positive element defines a translation invariant partial order on the set of self-adjoint elements {{nowrap|.}} If holds for , one writes or {{nowrap|.{{sfn|Palmer|2001|p=799}}}}
This partial order fulfills the properties and for all with {{nowrap| and .}}{{sfn|Palmer|2001|p=802}}
If is a C*-algebra, the partial order also has the following properties for :
- If holds, then is true for every {{nowrap|.}} For every that commutates with and even {{nowrap|holds.{{sfn|Kadison|Ringrose|1983|p=249}}}}
- If holds, then {{nowrap|.{{sfn|Kadison|Ringrose|1983|p=250}}}}
- If holds, then holds for all real numbers {{nowrap|.{{sfn|Blackadar|2006|p=66}}}}
- If is invertible and holds, then is invertible and for the inverses {{nowrap|holds.{{sfn|Kadison|Ringrose|1983|p=250}}}}
See also
Citations
=References=
{{reflist}}
= Bibliography =
{{refbegin|30em}}
- {{cite book |last=Blackadar|first=Bruce |title=Operator Algebras. Theory of C*-Algebras and von Neumann Algebras |publisher=Springer |location=Berlin/Heidelberg |year=2006 |isbn=3-540-28486-9 }}
- {{cite book |last=Dixmier |first=Jacques |title=C*-algebras |publisher=North-Holland |location=Amsterdam/New York/Oxford |year=1977 |isbn=0-7204-0762-1 |translator-last=Jellett |translator-first=Francis }} English translation of {{cite book |display-authors=0 |last=Dixmier |first=Jacques |title=Les C*-algèbres et leurs représentations |language=fr |publisher=Gauthier-Villars |year=1969 }}
- {{cite book |last1=Kadison |first1=Richard V. |last2=Ringrose |first2=John R. |title=Fundamentals of the Theory of Operator Algebras. Volume 1 Elementary Theory. |publisher=Academic Press |location=New York/London |year=1983 |isbn=0-12-393301-3}}
- {{cite book |last=Palmer|first=Theodore W. |title=Banach algebras and the general theory of*-algebras: Volume 2,*-algebras. |publisher=Cambridge university press |year=2001 |isbn=0-521-36638-0 }}
{{refend}}
{{SpectralTheory}}