Vector bornology

In mathematics, especially functional analysis, a bornology B {\displaystyle {\mathcal {B}}} on a vector space X {\displaystyle X} over a field K , {\displaystyle \mathbb {K} ,} where K {\displaystyle \mathbb {K} } has a bornology ℬ F {\displaystyle \mathbb {F} } , is called a vector bornology if B {\displaystyle {\mathcal {B}}} makes the vector space operations into bounded maps.

Definitions

Prerequisits

A bornology on a set X {\displaystyle X} is a collection B {\displaystyle {\mathcal {B}}} of subsets of X {\displaystyle X} that satisfy all the following conditions:

  1. B {\displaystyle {\mathcal {B}}} covers X ; {\displaystyle X;} that is, X = B {\displaystyle X=\cup {\mathcal {B}}}
  2. B {\displaystyle {\mathcal {B}}} is stable under inclusions; that is, if B B {\displaystyle B\in {\mathcal {B}}} and A B , {\displaystyle A\subseteq B,} then A B {\displaystyle A\in {\mathcal {B}}}
  3. B {\displaystyle {\mathcal {B}}} is stable under finite unions; that is, if B 1 , , B n B {\displaystyle B_{1},\ldots ,B_{n}\in {\mathcal {B}}} then B 1 B n B {\displaystyle B_{1}\cup \cdots \cup B_{n}\in {\mathcal {B}}}

Elements of the collection B {\displaystyle {\mathcal {B}}} are called B {\displaystyle {\mathcal {B}}} -bounded or simply bounded sets if B {\displaystyle {\mathcal {B}}} is understood. The pair ( X , B ) {\displaystyle (X,{\mathcal {B}})} is called a bounded structure or a bornological set.

A base or fundamental system of a bornology B {\displaystyle {\mathcal {B}}} is a subset B 0 {\displaystyle {\mathcal {B}}_{0}} of B {\displaystyle {\mathcal {B}}} such that each element of B {\displaystyle {\mathcal {B}}} is a subset of some element of B 0 . {\displaystyle {\mathcal {B}}_{0}.} Given a collection S {\displaystyle {\mathcal {S}}} of subsets of X , {\displaystyle X,} the smallest bornology containing S {\displaystyle {\mathcal {S}}} is called the bornology generated by S . {\displaystyle {\mathcal {S}}.} [1]

If ( X , B ) {\displaystyle (X,{\mathcal {B}})} and ( Y , C ) {\displaystyle (Y,{\mathcal {C}})} are bornological sets then their product bornology on X × Y {\displaystyle X\times Y} is the bornology having as a base the collection of all sets of the form B × C , {\displaystyle B\times C,} where B B {\displaystyle B\in {\mathcal {B}}} and C C . {\displaystyle C\in {\mathcal {C}}.} [1] A subset of X × Y {\displaystyle X\times Y} is bounded in the product bornology if and only if its image under the canonical projections onto X {\displaystyle X} and Y {\displaystyle Y} are both bounded.

If ( X , B ) {\displaystyle (X,{\mathcal {B}})} and ( Y , C ) {\displaystyle (Y,{\mathcal {C}})} are bornological sets then a function f : X Y {\displaystyle f:X\to Y} is said to be a locally bounded map or a bounded map (with respect to these bornologies) if it maps B {\displaystyle {\mathcal {B}}} -bounded subsets of X {\displaystyle X} to C {\displaystyle {\mathcal {C}}} -bounded subsets of Y ; {\displaystyle Y;} that is, if f ( B ) C . {\displaystyle f\left({\mathcal {B}}\right)\subseteq {\mathcal {C}}.} [1] If in addition f {\displaystyle f} is a bijection and f 1 {\displaystyle f^{-1}} is also bounded then f {\displaystyle f} is called a bornological isomorphism.

Vector bornology

Let X {\displaystyle X} be a vector space over a field K {\displaystyle \mathbb {K} } where K {\displaystyle \mathbb {K} } has a bornology B K . {\displaystyle {\mathcal {B}}_{\mathbb {K} }.} A bornology B {\displaystyle {\mathcal {B}}} on X {\displaystyle X} is called a vector bornology on X {\displaystyle X} if it is stable under vector addition, scalar multiplication, and the formation of balanced hulls (i.e. if the sum of two bounded sets is bounded, etc.).

If X {\displaystyle X} is a vector space and B {\displaystyle {\mathcal {B}}} is a bornology on X , {\displaystyle X,} then the following are equivalent:

  1. B {\displaystyle {\mathcal {B}}} is a vector bornology
  2. Finite sums and balanced hulls of B {\displaystyle {\mathcal {B}}} -bounded sets are B {\displaystyle {\mathcal {B}}} -bounded[1]
  3. The scalar multiplication map K × X X {\displaystyle \mathbb {K} \times X\to X} defined by ( s , x ) s x {\displaystyle (s,x)\mapsto sx} and the addition map X × X X {\displaystyle X\times X\to X} defined by ( x , y ) x + y , {\displaystyle (x,y)\mapsto x+y,} are both bounded when their domains carry their product bornologies (i.e. they map bounded subsets to bounded subsets)[1]

A vector bornology B {\displaystyle {\mathcal {B}}} is called a convex vector bornology if it is stable under the formation of convex hulls (i.e. the convex hull of a bounded set is bounded) then B . {\displaystyle {\mathcal {B}}.} And a vector bornology B {\displaystyle {\mathcal {B}}} is called separated if the only bounded vector subspace of X {\displaystyle X} is the 0-dimensional trivial space { 0 } . {\displaystyle \{0\}.}

Usually, K {\displaystyle \mathbb {K} } is either the real or complex numbers, in which case a vector bornology B {\displaystyle {\mathcal {B}}} on X {\displaystyle X} will be called a convex vector bornology if B {\displaystyle {\mathcal {B}}} has a base consisting of convex sets.

Characterizations

Suppose that X {\displaystyle X} is a vector space over the field F {\displaystyle \mathbb {F} } of real or complex numbers and B {\displaystyle {\mathcal {B}}} is a bornology on X . {\displaystyle X.} Then the following are equivalent:

  1. B {\displaystyle {\mathcal {B}}} is a vector bornology
  2. addition and scalar multiplication are bounded maps[1]
  3. the balanced hull of every element of B {\displaystyle {\mathcal {B}}} is an element of B {\displaystyle {\mathcal {B}}} and the sum of any two elements of B {\displaystyle {\mathcal {B}}} is again an element of B {\displaystyle {\mathcal {B}}} [1]

Bornology on a topological vector space

If X {\displaystyle X} is a topological vector space then the set of all bounded subsets of X {\displaystyle X} from a vector bornology on X {\displaystyle X} called the von Neumann bornology of X {\displaystyle X} , the usual bornology, or simply the bornology of X {\displaystyle X} and is referred to as natural boundedness.[1] In any locally convex topological vector space X , {\displaystyle X,} the set of all closed bounded disks form a base for the usual bornology of X . {\displaystyle X.} [1]

Unless indicated otherwise, it is always assumed that the real or complex numbers are endowed with the usual bornology.

Topology induced by a vector bornology

Suppose that X {\displaystyle X} is a vector space over the field K {\displaystyle \mathbb {K} } of real or complex numbers and B {\displaystyle {\mathcal {B}}} is a vector bornology on X . {\displaystyle X.} Let N {\displaystyle {\mathcal {N}}} denote all those subsets N {\displaystyle N} of X {\displaystyle X} that are convex, balanced, and bornivorous. Then N {\displaystyle {\mathcal {N}}} forms a neighborhood basis at the origin for a locally convex topological vector space topology.

Examples

Locally convex space of bounded functions

Let K {\displaystyle \mathbb {K} } be the real or complex numbers (endowed with their usual bornologies), let ( T , B ) {\displaystyle (T,{\mathcal {B}})} be a bounded structure, and let L B ( T , K ) {\displaystyle LB(T,\mathbb {K} )} denote the vector space of all locally bounded K {\displaystyle \mathbb {K} } -valued maps on T . {\displaystyle T.} For every B B , {\displaystyle B\in {\mathcal {B}},} let p B ( f ) := sup | f ( B ) | {\displaystyle p_{B}(f):=\sup \left|f(B)\right|} for all f L B ( T , K ) , {\displaystyle f\in LB(T,\mathbb {K} ),} where this defines a seminorm on X . {\displaystyle X.} The locally convex topological vector space topology on L B ( T , K ) {\displaystyle LB(T,\mathbb {K} )} defined by the family of seminorms { p B : B B } {\displaystyle \left\{p_{B}:B\in {\mathcal {B}}\right\}} is called the topology of uniform convergence on bounded set.[1] This topology makes L B ( T , K ) {\displaystyle LB(T,\mathbb {K} )} into a complete space.[1]

Bornology of equicontinuity

Let T {\displaystyle T} be a topological space, K {\displaystyle \mathbb {K} } be the real or complex numbers, and let C ( T , K ) {\displaystyle C(T,\mathbb {K} )} denote the vector space of all continuous K {\displaystyle \mathbb {K} } -valued maps on T . {\displaystyle T.} The set of all equicontinuous subsets of C ( T , K ) {\displaystyle C(T,\mathbb {K} )} forms a vector bornology on C ( T , K ) . {\displaystyle C(T,\mathbb {K} ).} [1]

See also

Citations

  1. ^ a b c d e f g h i j k l Narici & Beckenstein 2011, pp. 156–175.

Bibliography

  • Hogbe-Nlend, Henri (1977). Bornologies and Functional Analysis: Introductory Course on the Theory of Duality Topology-Bornology and its use in Functional Analysis. North-Holland Mathematics Studies. Vol. 26. Amsterdam New York New York: North Holland. ISBN 978-0-08-087137-0. MR 0500064. OCLC 316549583.
  • Kriegl, Andreas; Michor, Peter W. (1997). The Convenient Setting of Global Analysis. Mathematical Surveys and Monographs. American Mathematical Society. ISBN 978-082180780-4.
  • Narici, Lawrence; Beckenstein, Edward (2011). Topological Vector Spaces. Pure and applied mathematics (Second ed.). Boca Raton, FL: CRC Press. ISBN 978-1584888666. OCLC 144216834.
  • Schaefer, Helmut H.; Wolff, Manfred P. (1999). Topological Vector Spaces. GTM. Vol. 8 (Second ed.). New York, NY: Springer New York Imprint Springer. ISBN 978-1-4612-7155-0. OCLC 840278135.
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