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Dual system

In mathematics, a dual system, dual pair, or a duality over a field is a triple consisting of two vector spaces and over and a non-degenerate bilinear map .

Mathematical duality theory, the study of dual systems, has an important place in functional analysis and has extensive applications to quantum mechanics via the theory of Hilbert spaces.

Definition, notation, and conventions edit

Pairings edit

A pairing or pair over a field is a triple which may also be denoted by consisting of two vector spaces and over and a bilinear map , called the bilinear map associated with the pairing[1] or simply the pairing's map or its bilinear form. For simplicity, this article only covers examples where is either the real numbers or the complex numbers .

For every , define

and for every define
Every is a linear functional on and every is a linear functional on . Let
where each of these sets forms a vector space of linear functionals.

It is common practice to write instead of , in which case the pairing may often be denoted by rather than . However, this article will reserve the use of for the canonical evaluation map (defined below) so as to avoid confusion for readers not familiar with this subject.

Dual pairings edit

A pairing is called a dual system, a dual pair,[2] or a duality over if the bilinear form is non-degenerate, which means that it satisfies the following two separation axioms:

  1. separates (distinguishes) points of : if is such that then ; or equivalently, for all non-zero , the map is not identically (i.e. there exists a such that for each );
  2. separates (distinguishes) points of : if is such that then ; or equivalently, for all non-zero the map is not identically (i.e. there exists an such that for each ).

In this case is non-degenerate, and one can say that places and in duality (or, redundantly but explicitly, in separated duality), and is called the duality pairing of the triple .[1][2]

Total subsets edit

A subset of is called total if for every ,

implies A total subset of is defined analogously (see footnote).[note 1] Thus separates points of if and only if is a total subset of , and similarly for .

Orthogonality edit

The vectors and are called orthogonal, written , if . Two subsets and are orthogonal, written , if ; that is, if for all and . The definition of a subset being orthogonal to a vector is defined analogously.

The orthogonal complement or annihilator of a subset is

. Thus is a total subset of if and only if equals .

Polar sets edit

Given a triple defining a pairing over , the absolute polar set or polar set of a subset of is the set:

Symmetrically, the absolute polar set or polar set of a subset of is denoted by and defined by


To use bookkeeping that helps keep track of the antisymmetry of the two sides of the duality, the absolute polar of a subset of may also be called the absolute prepolar or prepolar of and then may be denoted by [3]

The polar is necessarily a convex set containing where if is balanced then so is and if is a vector subspace of then so too is a vector subspace of [4]

If is a vector subspace of then and this is also equal to the real polar of If then the bipolar of , denoted , is the polar of the orthogonal complement of , i.e., the set Similarly, if then the bipolar of is

Dual definitions and results edit

Given a pairing define a new pairing where for all and .[1]

There is a consistent theme in duality theory that any definition for a pairing has a corresponding dual definition for the pairing

Convention and Definition: Given any definition for a pairing one obtains a dual definition by applying it to the pairing This conventions also apply to theorems.

For instance, if " distinguishes points of " (resp, " is a total subset of ") is defined as above, then this convention immediately produces the dual definition of " distinguishes points of " (resp, " is a total subset of ").

This following notation is almost ubiquitous and allows us to avoid assigning a symbol to

Convention and Notation: If a definition and its notation for a pairing depends on the order of and (for example, the definition of the Mackey topology on ) then by switching the order of and then it is meant that definition applied to (continuing the same example, the topology would actually denote the topology ).

For another example, once the weak topology on is defined, denoted by , then this dual definition would automatically be applied to the pairing so as to obtain the definition of the weak topology on , and this topology would be denoted by rather than .

Identification of with edit

Although it is technically incorrect and an abuse of notation, this article will adhere to the nearly ubiquitous convention of treating a pairing interchangeably with and also of denoting by

Examples edit

Restriction of a pairing edit

Suppose that is a pairing, is a vector subspace of and is a vector subspace of . Then the restriction of to is the pairing If is a duality, then it's possible for a restriction to fail to be a duality (e.g. if and ).

This article will use the common practice of denoting the restriction by

Canonical duality on a vector space edit

Suppose that is a vector space and let denote the algebraic dual space of (that is, the space of all linear functionals on ). There is a canonical duality where which is called the evaluation map or the natural or canonical bilinear functional on Note in particular that for any is just another way of denoting ; i.e.

If is a vector subspace of , then the restriction of to is called the canonical pairing where if this pairing is a duality then it is instead called the canonical duality. Clearly, always distinguishes points of , so the canonical pairing is a dual system if and only if separates points of The following notation is now nearly ubiquitous in duality theory.

The evaluation map will be denoted by (rather than by ) and will be written rather than

Assumption: As is common practice, if is a vector space and is a vector space of linear functionals on then unless stated otherwise, it will be assumed that they are associated with the canonical pairing

If is a vector subspace of then distinguishes points of (or equivalently, is a duality) if and only if distinguishes points of or equivalently if is total (that is, for all implies ).[1]

Canonical duality on a topological vector space edit

Suppose is a topological vector space (TVS) with continuous dual space Then the restriction of the canonical duality to × defines a pairing for which separates points of If separates points of (which is true if, for instance, is a Hausdorff locally convex space) then this pairing forms a duality.[2]

Assumption: As is commonly done, whenever is a TVS, then unless indicated otherwise, it will be assumed without comment that it's associated with the canonical pairing

Polars and duals of TVSs edit

The following result shows that the continuous linear functionals on a TVS are exactly those linear functionals that are bounded on a neighborhood of the origin.

Theorem[1] — Let be a TVS with algebraic dual and let be a basis of neighborhoods of at the origin. Under the canonical duality the continuous dual space of is the union of all as ranges over (where the polars are taken in ).

Inner product spaces and complex conjugate spaces edit

A pre-Hilbert space is a dual pairing if and only if is vector space over or has dimension Here it is assumed that the sesquilinear form is conjugate homogeneous in its second coordinate and homogeneous in its first coordinate.

  • If is a real Hilbert space then forms a dual system.
  • If is a complex Hilbert space then forms a dual system if and only if If is non-trivial then does not even form pairing since the inner product is sesquilinear rather than bilinear.[1]

Suppose that is a complex pre-Hilbert space with scalar multiplication denoted as usual by juxtaposition or by a dot Define the map

where the right-hand side uses the scalar multiplication of Let denote the complex conjugate vector space of where denotes the additive group of (so vector addition in is identical to vector addition in ) but with scalar multiplication in being the map (instead of the scalar multiplication that is endowed with).

The map defined by is linear in both coordinates[note 2] and so forms a dual pairing.

Other examples edit

  • Suppose and for all let
    Then is a pairing such that distinguishes points of but does not distinguish points of Furthermore,
  • Let (where is such that ), and Then is a dual system.
  • Let and be vector spaces over the same field Then the bilinear form places and in duality.[2]
  • A sequence space and its beta dual with the bilinear map defined as for forms a dual system.

Weak topology edit

Suppose that is a pairing of vector spaces over If then the weak topology on induced by (and ) is the weakest TVS topology on denoted by or simply making all maps continuous as ranges over [1] If is not clear from context then it should be assumed to be all of in which case it is called the weak topology on (induced by ). The notation or (if no confusion could arise) simply is used to denote endowed with the weak topology Importantly, the weak topology depends entirely on the function the usual topology on and 's vector space structure but not on the algebraic structures of

Similarly, if then the dual definition of the weak topology on induced by (and ), which is denoted by or simply (see footnote for details).[note 3]

Definition and Notation: If "" is attached to a topological definition (e.g. -converges, -bounded, etc.) then it means that definition when the first space (i.e. ) carries the topology. Mention of or even and may be omitted if no confusion arises. So, for instance, if a sequence in "-converges" or "weakly converges" then this means that it converges in whereas if it were a sequence in , then this would mean that it converges in ).

The topology is locally convex since it is determined by the family of seminorms defined by as ranges over [1] If and is a net in then -converges to if converges to in [1] A net -converges to if and only if for all converges to If is a sequence of orthonormal vectors in Hilbert space, then converges weakly to 0 but does not norm-converge to 0 (or any other vector).[1]

If is a pairing and is a proper vector subspace of such that is a dual pair, then is strictly coarser than [1]

Bounded subsets edit

A subset of is -bounded if and only if

where

Hausdorffness edit

If is a pairing then the following are equivalent:

  1. distinguishes points of ;
  2. The map defines an injection from into the algebraic dual space of ;[1]
  3. is Hausdorff.[1]

Weak representation theorem edit

The following theorem is of fundamental importance to duality theory because it completely characterizes the continuous dual space of

Weak representation theorem[1] — Let be a pairing over the field Then the continuous dual space of is

Furthermore,

  1. If is a continuous linear functional on then there exists some such that ; if such a exists then it is unique if and only if distinguishes points of
    • Note that whether or not distinguishes points of is not dependent on the particular choice of
  2. The continuous dual space of may be identified with the quotient space where
    • This is true regardless of whether or not distinguishes points of or distinguishes points of

Consequently, the continuous dual space of is

With respect to the canonical pairing, if is a TVS whose continuous dual space separates points on (i.e. such that is Hausdorff, which implies that is also necessarily Hausdorff) then the continuous dual space of is equal to the set of all "evaluation at a point " maps as ranges over (i.e. the map that send to ). This is commonly written as

This very important fact is why results for polar topologies on continuous dual spaces, such as the strong dual topology on for example, can also often be applied to the original TVS ; for instance, being identified with means that the topology on can instead be thought of as a topology on Moreover, if is endowed with a topology that is finer than then the continuous dual space of will necessarily contain as a subset. So for instance, when is endowed with the strong dual topology (and so is denoted by ) then
which (among other things) allows for to be endowed with the subspace topology induced on it by, say, the strong dual topology (this topology is also called the strong bidual topology and it appears in the theory of reflexive spaces: the Hausdorff locally convex TVS is said to be semi-reflexive if and it will be called reflexive if in addition the strong bidual topology on is equal to 's original/starting topology).

Orthogonals, quotients, and subspaces edit

If is a pairing then for any subset of :

  • and this set is -closed;[1]
  • ;[1]
    • Thus if is a -closed vector subspace of then
  • If is a family of -closed vector subspaces of then
    [1]
  • If is a family of subsets of then [1]

If is a normed space then under the canonical duality, is norm closed in and is norm closed in [1]

Subspaces edit

Suppose that is a vector subspace of and let denote the restriction of to The weak topology on is identical to the subspace topology that inherits from

Also, is a paired space (where means ) where is defined by

The topology is equal to the subspace topology that inherits from [5] Furthermore, if is a dual system then so is [5]

Quotients edit

Suppose that is a vector subspace of Then is a paired space where is defined by

The topology is identical to the usual quotient topology induced by on [5]

Polars and the weak topology edit

If is a locally convex space and if is a subset of the continuous dual space then is -bounded if and only if for some barrel in [1]

The following results are important for defining polar topologies.

If is a pairing and then:[1]

  1. The polar of is a closed subset of
  2. The polars of the following sets are identical: (a) ; (b) the convex hull of ; (c) the balanced hull of ; (d) the -closure of ; (e) the -closure of the convex balanced hull of
  3. The bipolar theorem: The bipolar of denoted by is equal to the -closure of the convex balanced hull of
    • The bipolar theorem in particular "is an indispensable tool in working with dualities."[4]
  4. is -bounded if and only if is absorbing in
  5. If in addition distinguishes points of then is -bounded if and only if it is -totally bounded.

If is a pairing and is a locally convex topology on that is consistent with duality, then a subset of is a barrel in if and only if is the polar of some -bounded subset of [6]

Transposes edit

Transposes of a linear map with respect to pairings edit

Let and be pairings over and let be a linear map.

For all let be the map defined by It is said that 's transpose or adjoint is well-defined if the following conditions are satisfied:

  1. distinguishes points of (or equivalently, the map from into the algebraic dual is injective), and
  2. where and .

In this case, for any

dual, system, this, article, about, dual, pairs, vector, spaces, dual, pairs, representation, theory, reductive, dual, pair, this, reads, like, textbook, encyclopedia, tone, style, reflect, encyclopedic, tone, used, wikipedia, wikipedia, guide, writing, better. This article is about dual pairs of vector spaces For dual pairs in representation theory see Reductive dual pair This reads like a textbook not an encyclopedia s tone or style may not reflect the encyclopedic tone used on Wikipedia See Wikipedia s guide to writing better articles for suggestions January 2022 Learn how and when to remove this template message In mathematics a dual system dual pair or a duality over a field K displaystyle mathbb K is a triple X Y b displaystyle X Y b consisting of two vector spaces X displaystyle X and Y displaystyle Y over K displaystyle mathbb K and a non degenerate bilinear map b X x00D7 Y x2192 K displaystyle b X times Y to mathbb K Mathematical duality theory the study of dual systems has an important place in functional analysis and has extensive applications to quantum mechanics via the theory of Hilbert spaces Contents 1 Definition notation and conventions 1 1 Pairings 1 2 Dual pairings 1 3 Total subsets 1 4 Orthogonality 1 5 Polar sets 1 6 Dual definitions and results 1 6 1 Identification of UNIQ postMath 0000009D QINU with UNIQ postMath 0000009E QINU 2 Examples 2 1 Restriction of a pairing 2 2 Canonical duality on a vector space 2 3 Canonical duality on a topological vector space 2 4 Polars and duals of TVSs 2 5 Inner product spaces and complex conjugate spaces 2 6 Other examples 3 Weak topology 3 1 Bounded subsets 3 2 Hausdorffness 3 3 Weak representation theorem 3 4 Orthogonals quotients and subspaces 3 5 Subspaces 3 6 Quotients 3 7 Polars and the weak topology 4 Transposes 4 1 Transposes of a linear map with respect to pairings 4 2 Properties of the transpose 4 2 1 Weak continuity 4 3 Weak topology and the canonical duality 4 3 1 Weak completeness 4 3 2 Identification of Y with a subspace of the algebraic dual 4 3 3 Algebraic adjoint 4 3 4 Weak continuity and openness 4 3 4 1 Transpose of a map between TVSs 4 3 5 Metrizability and separability 5 Polar topologies and topologies compatible with pairing 5 1 Polar topologies 5 1 1 Definitions involving polar topologies 5 2 Bounded subsets 5 3 Topologies compatible with a pair 5 3 1 Mackey Arens theorem 5 4 Mackey s theorem barrels and closed convex sets 5 5 Space of finite sequences 6 See also 7 Notes 8 References 9 Bibliography 10 External links Definition notation and conventions edit Pairings edit A pairing or pair over a field K displaystyle mathbb K is a triple X Y b displaystyle X Y b which may also be denoted by b X Y displaystyle b X Y consisting of two vector spaces X displaystyle X and Y displaystyle Y over K displaystyle mathbb K and a bilinear map b X x00D7 Y x2192 K displaystyle b X times Y to mathbb K called the bilinear map associated with the pairing 91 1 93 or simply the pairing s map or its bilinear form For simplicity this article only covers examples where K displaystyle mathbb K is either the real numbers R displaystyle mathbb R or the complex numbers C displaystyle mathbb C For every x x2208 X displaystyle x in X define b x x22C5 Y x2192 K y x21A6 b x y displaystyle begin alignedat 4 b x cdot amp Y amp amp to amp amp mathbb K amp y amp amp mapsto amp amp b x y end alignedat and for every y x2208 Y displaystyle y in Y define b x22C5 y X x2192 K x x21A6 b x y displaystyle begin alignedat 4 b cdot y amp X amp amp to amp amp mathbb K amp x amp amp mapsto amp amp b x y end alignedat Every b x x22C5 displaystyle b x cdot is a linear functional on Y displaystyle Y and every b x22C5 y displaystyle b cdot y is a linear functional on X displaystyle X Let b X x22C5 b x x22C5 x x2208 X xA0 and xA0 b x22C5 Y b x22C5 y y x2208 Y displaystyle b X cdot b x cdot x in X qquad text and qquad b cdot Y b cdot y y in Y where each of these sets forms a vector space of linear functionals It is common practice to write x27E8 x y x27E9 displaystyle langle x y rangle instead of b x y displaystyle b x y in which case the pairing may often be denoted by x27E8 X Y x27E9 displaystyle left langle X Y right rangle rather than X Y x27E8 x22C5 x22C5 x27E9 displaystyle X Y langle cdot cdot rangle However this article will reserve the use of x27E8 x22C5 x22C5 x27E9 displaystyle langle cdot cdot rangle for the canonical evaluation map defined below so as to avoid confusion for readers not familiar with this subject Dual pairings edit A pairing X Y b displaystyle X Y b is called a dual system a dual pair 91 2 93 or a duality over K displaystyle mathbb K if the bilinear form b displaystyle b is non degenerate which means that it satisfies the following two separation axioms Y displaystyle Y separates distinguishes points of X displaystyle X if x x2208 X displaystyle x in X is such that b x x22C5 0 displaystyle b x cdot 0 then x 0 displaystyle x 0 or equivalently for all non zero x x2208 X displaystyle x in X the map b x x22C5 Y x2192 K displaystyle b x cdot Y to mathbb K is not identically 0 displaystyle 0 i e there exists a y x2208 Y displaystyle y in Y such that b x y x2260 0 displaystyle b x y neq 0 for each x x2208 X displaystyle x in X X displaystyle X separates distinguishes points of Y displaystyle Y if y x2208 Y displaystyle y in Y is such that b x22C5 y 0 displaystyle b cdot y 0 then y 0 displaystyle y 0 or equivalently for all non zero y x2208 Y displaystyle y in Y the map b x22C5 y X x2192 K displaystyle b cdot y X to mathbb K is not identically 0 displaystyle 0 i e there exists an x x2208 X displaystyle x in X such that b x y x2260 0 displaystyle b x y neq 0 for each y x2208 Y displaystyle y in Y In this case b displaystyle b is non degenerate and one can say that b displaystyle b places X displaystyle X and Y displaystyle Y in duality or redundantly but explicitly in separated duality and b displaystyle b is called the duality pairing of the triple X Y b displaystyle X Y b 91 1 93 91 2 93 Total subsets edit A subset S displaystyle S of Y displaystyle Y is called total if for every x x2208 X displaystyle x in X b x s 0 xA0 for all xA0 s x2208 S displaystyle b x s 0 quad text for all s in S implies x 0 displaystyle x 0 A total subset of X displaystyle X is defined analogously see footnote 91 note 1 93 Thus X displaystyle X separates points of Y displaystyle Y if and only if X displaystyle X is a total subset of X displaystyle X and similarly for Y displaystyle Y Orthogonality edit The vectors x displaystyle x and y displaystyle y are called orthogonal written x x22A5 y displaystyle x perp y if b x y 0 displaystyle b x y 0 Two subsets R x2286 X displaystyle R subseteq X and S x2286 Y displaystyle S subseteq Y are orthogonal written R x22A5 S displaystyle R perp S if b R S 0 displaystyle b R S 0 that is if b r s 0 displaystyle b r s 0 for all r x2208 R displaystyle r in R and s x2208 S displaystyle s in S The definition of a subset being orthogonal to a vector is defined analogously The orthogonal complement or annihilator of a subset R x2286 X displaystyle R subseteq X is R x22A5 y x2208 Y R x22A5 y y x2208 Y b R y 0 displaystyle R perp y in Y R perp y y in Y b R y 0 Thus R displaystyle R is a total subset of X displaystyle X if and only if R x22A5 displaystyle R perp equals 0 displaystyle 0 Polar sets edit Main article Polar set Given a triple X Y b displaystyle X Y b defining a pairing over K displaystyle mathbb K the absolute polar set or polar set of a subset A displaystyle A of X displaystyle X is the set A x2218 y x2208 Y sup x x2208 A b x y x2264 1 displaystyle A circ left y in Y sup x in A b x y leq 1 right Symmetrically the absolute polar set or polar set of a subset B displaystyle B of Y displaystyle Y is denoted by B x2218 displaystyle B circ and defined by B x2218 x x2208 X sup y x2208 B b x y x2264 1 displaystyle B circ left x in X sup y in B b x y leq 1 right To use bookkeeping that helps keep track of the antisymmetry of the two sides of the duality the absolute polar of a subset B displaystyle B of Y displaystyle Y may also be called the absolute prepolar or prepolar of B displaystyle B and then may be denoted by x2218 B displaystyle circ B 91 3 93 The polar B x2218 displaystyle B circ is necessarily a convex set containing 0 x2208 Y displaystyle 0 in Y where if B displaystyle B is balanced then so is B x2218 displaystyle B circ and if B displaystyle B is a vector subspace of X displaystyle X then so too is B x2218 displaystyle B circ a vector subspace of Y displaystyle Y 91 4 93 If A displaystyle A is a vector subspace of X displaystyle X then A x2218 A x22A5 displaystyle A circ A perp and this is also equal to the real polar of A displaystyle A If A x2286 X displaystyle A subseteq X then the bipolar of A displaystyle A denoted A x2218 x2218 displaystyle A circ circ is the polar of the orthogonal complement of A displaystyle A i e the set x2218 A x22A5 displaystyle circ left A perp right Similarly if B x2286 Y displaystyle B subseteq Y then the bipolar of B displaystyle B is B x2218 x2218 x2218 B x2218 displaystyle B circ circ left circ B right circ Dual definitions and results edit Given a pairing X Y b displaystyle X Y b define a new pairing Y X d displaystyle Y X d where d y x b x y displaystyle d y x b x y for all x x2208 X displaystyle x in X and y x2208 Y displaystyle y in Y 91 1 93 There is a consistent theme in duality theory that any definition for a pairing X Y b displaystyle X Y b has a corresponding dual definition for the pairing Y X d displaystyle Y X d Convention and Definition Given any definition for a pairing X Y b displaystyle X Y b one obtains a dual definition by applying it to the pairing Y X d displaystyle Y X d This conventions also apply to theorems For instance if X displaystyle X distinguishes points of Y displaystyle Y resp S displaystyle S is a total subset of Y displaystyle Y is defined as above then this convention immediately produces the dual definition of Y displaystyle Y distinguishes points of X displaystyle X resp S displaystyle S is a total subset of X displaystyle X This following notation is almost ubiquitous and allows us to avoid assigning a symbol to d displaystyle d Convention and Notation If a definition and its notation for a pairing X Y b displaystyle X Y b depends on the order of X displaystyle X and Y displaystyle Y for example the definition of the Mackey topology x03C4 X Y b displaystyle tau X Y b on X displaystyle X then by switching the order of X displaystyle X and Y displaystyle Y then it is meant that definition applied to Y X d displaystyle Y X d continuing the same example the topology x03C4 Y X b displaystyle tau Y X b would actually denote the topology x03C4 Y X d displaystyle tau Y X d For another example once the weak topology on X displaystyle X is defined denoted by x03C3 X Y b displaystyle sigma X Y b then this dual definition would automatically be applied to the pairing Y X d displaystyle Y X d so as to obtain the definition of the weak topology on Y displaystyle Y and this topology would be denoted by x03C3 Y X b displaystyle sigma Y X b rather than x03C3 Y X d displaystyle sigma Y X d Identification of X Y displaystyle X Y with Y X displaystyle Y X edit Although it is technically incorrect and an abuse of notation this article will adhere to the nearly ubiquitous convention of treating a pairing X Y b displaystyle X Y b interchangeably with Y X d displaystyle Y X d and also of denoting Y X d displaystyle Y X d by Y X b displaystyle Y X b Examples edit Restriction of a pairing edit Suppose that X Y b displaystyle X Y b is a pairing M displaystyle M is a vector subspace of X displaystyle X and N displaystyle N is a vector subspace of Y displaystyle Y Then the restriction of X Y b displaystyle X Y b to M x00D7 N displaystyle M times N is the pairing M N b M x00D7 N displaystyle left M N b big vert M times N right If X Y b displaystyle X Y b is a duality then it s possible for a restriction to fail to be a duality e g if Y x2260 0 displaystyle Y neq 0 and N 0 displaystyle N 0 This article will use the common practice of denoting the restriction M N b M x00D7 N displaystyle left M N b big vert M times N right by M N b displaystyle M N b Canonical duality on a vector space edit Suppose that X displaystyle X is a vector space and let X x0023 displaystyle X denote the algebraic dual space of X displaystyle X that is the space of all linear functionals on X displaystyle X There is a canonical duality X X x0023 c displaystyle left X X c right where c x x x2032 x27E8 x x x2032 x27E9 x x2032 x displaystyle c left x x prime right left langle x x prime right rangle x prime x which is called the evaluation map or the natural or canonical bilinear functional on X x00D7 X x0023 displaystyle X times X Note in particular that for any x x2032 x2208 X x0023 displaystyle x prime in X c x22C5 x x2032 displaystyle c left cdot x prime right is just another way of denoting x x2032 displaystyle x prime i e c x22C5 x x2032 x x2032 x22C5 x x2032 displaystyle c left cdot x prime right x prime cdot x prime If N displaystyle N is a vector subspace of X x0023 displaystyle X then the restriction of X X x0023 c displaystyle left X X c right to X x00D7 N displaystyle X times N is called the canonical pairing where if this pairing is a duality then it is instead called the canonical duality Clearly X displaystyle X always distinguishes points of N displaystyle N so the canonical pairing is a dual system if and only if N displaystyle N separates points of X displaystyle X The following notation is now nearly ubiquitous in duality theory The evaluation map will be denoted by x27E8 x x x2032 x27E9 x x2032 x displaystyle left langle x x prime right rangle x prime x rather than by c displaystyle c and x27E8 X N x27E9 displaystyle langle X N rangle will be written rather than X N c displaystyle X N c Assumption As is common practice if X displaystyle X is a vector space and N displaystyle N is a vector space of linear functionals on X displaystyle X then unless stated otherwise it will be assumed that they are associated with the canonical pairing x27E8 X N x27E9 displaystyle langle X N rangle If N displaystyle N is a vector subspace of X x0023 displaystyle X then X displaystyle X distinguishes points of N displaystyle N or equivalently X N c displaystyle X N c is a duality if and only if N displaystyle N distinguishes points of X displaystyle X or equivalently if N displaystyle N is total that is n x 0 displaystyle n x 0 for all n x2208 N displaystyle n in N implies x 0 displaystyle x 0 91 1 93 Canonical duality on a topological vector space edit Suppose X displaystyle X is a topological vector space TVS with continuous dual space X x2032 displaystyle X prime Then the restriction of the canonical duality X X x0023 c displaystyle left X X c right to X displaystyle X X x2032 displaystyle X prime defines a pairing X X x2032 c X x00D7 X x2032 displaystyle left X X prime c big vert X times X prime right for which X displaystyle X separates points of X x2032 displaystyle X prime If X x2032 displaystyle X prime separates points of X displaystyle X which is true if for instance X displaystyle X is a Hausdorff locally convex space then this pairing forms a duality 91 2 93 Assumption As is commonly done whenever X displaystyle X is a TVS then unless indicated otherwise it will be assumed without comment that it s associated with the canonical pairing x27E8 X X x2032 x27E9 displaystyle left langle X X prime right rangle Polars and duals of TVSs edit The following result shows that the continuous linear functionals on a TVS are exactly those linear functionals that are bounded on a neighborhood of the origin Theorem 91 1 93 160 8212 160 Let X displaystyle X be a TVS with algebraic dual X x0023 displaystyle X and let N displaystyle mathcal N be a basis of neighborhoods of X displaystyle X at the origin Under the canonical duality x27E8 X X x0023 x27E9 displaystyle left langle X X right rangle the continuous dual space of X displaystyle X is the union of all N x2218 displaystyle N circ as N displaystyle N ranges over N displaystyle mathcal N where the polars are taken in X x0023 displaystyle X Inner product spaces and complex conjugate spaces edit A pre Hilbert space H x27E8 x22C5 x22C5 x27E9 displaystyle H langle cdot cdot rangle is a dual pairing if and only if H displaystyle H is vector space over R displaystyle mathbb R or H displaystyle H has dimension 0 displaystyle 0 Here it is assumed that the sesquilinear form x27E8 x22C5 x22C5 x27E9 displaystyle langle cdot cdot rangle is conjugate homogeneous in its second coordinate and homogeneous in its first coordinate If H x27E8 x22C5 x22C5 x27E9 displaystyle H langle cdot cdot rangle is a real Hilbert space then H H x27E8 x22C5 x22C5 x27E9 displaystyle H H langle cdot cdot rangle forms a dual system If H x27E8 x22C5 x22C5 x27E9 displaystyle H langle cdot cdot rangle is a complex Hilbert space then H H x27E8 x22C5 x22C5 x27E9 displaystyle H H langle cdot cdot rangle forms a dual system if and only if dim x2061 H 0 displaystyle operatorname dim H 0 If H displaystyle H is non trivial then H H x27E8 x22C5 x22C5 x27E9 displaystyle H H langle cdot cdot rangle does not even form pairing since the inner product is sesquilinear rather than bilinear 91 1 93 Suppose that H x27E8 x22C5 x22C5 x27E9 displaystyle H langle cdot cdot rangle is a complex pre Hilbert space with scalar multiplication denoted as usual by juxtaposition or by a dot x22C5 displaystyle cdot Define the map x22C5 x22A5 x22C5 C x00D7 H x2192 H xA0 by xA0 c x22A5 x c x00AF x displaystyle cdot perp cdot mathbb C times H to H quad text by quad c perp x overline c x where the right hand side uses the scalar multiplication of H displaystyle H Let H x00AF displaystyle overline H denote the complex conjugate vector space of H displaystyle H where H x00AF displaystyle overline H denotes the additive group of H displaystyle H so vector addition in H x00AF displaystyle overline H is identical to vector addition in H displaystyle H but with scalar multiplication in H x00AF displaystyle overline H being the map x22C5 x22A5 x22C5 displaystyle cdot perp cdot instead of the scalar multiplication that H displaystyle H is endowed with The map b H x00D7 H x00AF x2192 C displaystyle b H times overline H to mathbb C defined by b x y x27E8 x y x27E9 displaystyle b x y langle x y rangle is linear in both coordinates 91 note 2 93 and so H H x00AF x27E8 x22C5 x22C5 x27E9 displaystyle left H overline H langle cdot cdot rangle right forms a dual pairing Other examples edit Suppose X R 2 displaystyle X mathbb R 2 Y R 3 displaystyle Y mathbb R 3 and for all x 1 y 1 x2208 X xA0 and xA0 x 2 y 2 z 2 x2208 Y displaystyle left x 1 y 1 right in X text and left x 2 y 2 z 2 right in Y let b x 1 y 1 x 2 y 2 z 2 x 1 x 2 y 1 y 2 displaystyle b left left x 1 y 1 right left x 2 y 2 z 2 right right x 1 x 2 y 1 y 2 Then X Y b displaystyle X Y b is a pairing such that X displaystyle X distinguishes points of Y displaystyle Y but Y displaystyle Y does not distinguish points of X displaystyle X Furthermore X x22A5 y x2208 Y X x22A5 y 0 0 z z x2208 R displaystyle X perp y in Y X perp y 0 0 z z in mathbb R Let 0 lt p lt x221E displaystyle 0 lt p lt infty X L p x03BC displaystyle X L p mu Y L q x03BC displaystyle Y L q mu where q displaystyle q is such that 1 p 1 q 1 displaystyle tfrac 1 p tfrac 1 q 1 and b f g x222B f g d x03BC displaystyle b f g int fg mathrm d mu Then X Y b displaystyle X Y b is a dual system Let X displaystyle X and Y displaystyle Y be vector spaces over the same field K displaystyle mathbb K Then the bilinear form b x x2297 y x x2217 x2297 y x2217 x27E8 x x2032 x x27E9 x27E8 y x2032 y x27E9 displaystyle b left x otimes y x otimes y right left langle x prime x right rangle left langle y prime y right rangle places X x00D7 Y displaystyle X times Y and X x0023 x00D7 Y x0023 displaystyle X times Y in duality 91 2 93 A sequence space X displaystyle X and its beta dual Y X x03B2 displaystyle Y X beta with the bilinear map defined as x27E8 x y x27E9 x2211 i 1 x221E x i y i displaystyle langle x y rangle sum i 1 infty x i y i for x x2208 X displaystyle x in X y x2208 X x03B2 displaystyle y in X beta forms a dual system Weak topology edit Main articles Weak topology and Weak topology Suppose that X Y b displaystyle X Y b is a pairing of vector spaces over K displaystyle mathbb K If S x2286 Y displaystyle S subseteq Y then the weak topology on X displaystyle X induced by S displaystyle S and b displaystyle b is the weakest TVS topology on X displaystyle X denoted by x03C3 X S b displaystyle sigma X S b or simply x03C3 X S displaystyle sigma X S making all maps b x22C5 y X x2192 K displaystyle b cdot y X to mathbb K continuous as y displaystyle y ranges over S displaystyle S 91 1 93 If S displaystyle S is not clear from context then it should be assumed to be all of Y displaystyle Y in which case it is called the weak topology on X displaystyle X induced by Y displaystyle Y The notation X x03C3 X S b displaystyle X sigma X S b X x03C3 X S displaystyle X sigma X S or if no confusion could arise simply X x03C3 displaystyle X sigma is used to denote X displaystyle X endowed with the weak topology x03C3 X S b displaystyle sigma X S b Importantly the weak topology depends entirely on the function b displaystyle b the usual topology on C displaystyle mathbb C and X displaystyle X s vector space structure but not on the algebraic structures of Y displaystyle Y Similarly if R x2286 X displaystyle R subseteq X then the dual definition of the weak topology on Y displaystyle Y induced by R displaystyle R and b displaystyle b which is denoted by x03C3 Y R b displaystyle sigma Y R b or simply x03C3 Y R displaystyle sigma Y R see footnote for details 91 note 3 93 Definition and Notation If x03C3 X Y b displaystyle sigma X Y b is attached to a topological definition e g x03C3 X Y b displaystyle sigma X Y b converges x03C3 X Y b displaystyle sigma X Y b bounded cl x03C3 X Y b x2061 S displaystyle operatorname cl sigma X Y b S etc then it means that definition when the first space i e X displaystyle X carries the x03C3 X Y b displaystyle sigma X Y b topology Mention of b displaystyle b or even X displaystyle X and Y displaystyle Y may be omitted if no confusion arises So for instance if a sequence a i i 1 x221E displaystyle left a i right i 1 infty in Y displaystyle Y x03C3 displaystyle sigma converges or weakly converges then this means that it converges in Y x03C3 Y X b displaystyle Y sigma Y X b whereas if it were a sequence in X displaystyle X then this would mean that it converges in X x03C3 X Y b displaystyle X sigma X Y b The topology x03C3 X Y b displaystyle sigma X Y b is locally convex since it is determined by the family of seminorms p y X x2192 R displaystyle p y X to mathbb R defined by p y x b x y displaystyle p y x b x y as y displaystyle y ranges over Y displaystyle Y 91 1 93 If x x2208 X displaystyle x in X and x i i x2208 I displaystyle left x i right i in I is a net in X displaystyle X then x i i x2208 I displaystyle left x i right i in I x03C3 X Y b displaystyle sigma X Y b converges to x displaystyle x if x i i x2208 I displaystyle left x i right i in I converges to x displaystyle x in X x03C3 X Y b displaystyle X sigma X Y b 91 1 93 A net x i i x2208 I displaystyle left x i right i in I x03C3 X Y b displaystyle sigma X Y b converges to x displaystyle x if and only if for all y x2208 Y displaystyle y in Y b x i y displaystyle b left x i y right converges to b x y displaystyle b x y If x i i 1 x221E displaystyle left x i right i 1 infty is a sequence of orthonormal vectors in Hilbert space then x i i 1 x221E displaystyle left x i right i 1 infty converges weakly to 0 but does not norm converge to 0 or any other vector 91 1 93 If X Y b displaystyle X Y b is a pairing and N displaystyle N is a proper vector subspace of Y displaystyle Y such that X N b displaystyle X N b is a dual pair then x03C3 X N b displaystyle sigma X N b is strictly coarser than x03C3 X Y b displaystyle sigma X Y b 91 1 93 Bounded subsets edit A subset S displaystyle S of X displaystyle X is x03C3 X Y b displaystyle sigma X Y b bounded if and only if sup b S y lt x221E xA0 for all xA0 y x2208 Y displaystyle sup b S y lt infty quad text for all y in Y where b S y b s y s x2208 S displaystyle b S y b s y s in S Hausdorffness edit If X Y b displaystyle X Y b is a pairing then the following are equivalent X displaystyle X distinguishes points of Y displaystyle Y The map y x21A6 b x22C5 y displaystyle y mapsto b cdot y defines an injection from Y displaystyle Y into the algebraic dual space of X displaystyle X 91 1 93 x03C3 Y X b displaystyle sigma Y X b is Hausdorff 91 1 93 Weak representation theorem edit The following theorem is of fundamental importance to duality theory because it completely characterizes the continuous dual space of X x03C3 X Y b displaystyle X sigma X Y b Weak representation theorem 91 1 93 160 8212 160 Let X Y b displaystyle X Y b be a pairing over the field K displaystyle mathbb K Then the continuous dual space of X x03C3 X Y b displaystyle X sigma X Y b is b x22C5 Y b x22C5 y y x2208 Y displaystyle b cdot Y b cdot y y in Y Furthermore If f displaystyle f is a continuous linear functional on X x03C3 X Y b displaystyle X sigma X Y b then there exists some y x2208 Y displaystyle y in Y such that f b x22C5 y displaystyle f b cdot y if such a y displaystyle y exists then it is unique if and only if X displaystyle X distinguishes points of Y displaystyle Y Note that whether or not X displaystyle X distinguishes points of Y displaystyle Y is not dependent on the particular choice of y displaystyle y The continuous dual space of X x03C3 X Y b displaystyle X sigma X Y b may be identified with the quotient space Y X x22A5 displaystyle Y X perp where X x22A5 y x2208 Y b x y 0 xA0 for all xA0 x x2208 X displaystyle X perp y in Y b x y 0 text for all x in X This is true regardless of whether or not X displaystyle X distinguishes points of Y displaystyle Y or Y displaystyle Y distinguishes points of X displaystyle X Consequently the continuous dual space of X x03C3 X Y b displaystyle X sigma X Y b is X x03C3 X Y b x2032 b x22C5 Y b x22C5 y y x2208 Y displaystyle X sigma X Y b prime b cdot Y left b cdot y y in Y right With respect to the canonical pairing if X displaystyle X is a TVS whose continuous dual space X x2032 displaystyle X prime separates points on X displaystyle X i e such that X x03C3 X X x2032 displaystyle left X sigma left X X prime right right is Hausdorff which implies that X displaystyle X is also necessarily Hausdorff then the continuous dual space of X x2032 x03C3 X x2032 X displaystyle left X prime sigma left X prime X right right is equal to the set of all evaluation at a point x displaystyle x maps as x displaystyle x ranges over X displaystyle X i e the map that send x x2032 x2208 X x2032 displaystyle x prime in X prime to x x2032 x displaystyle x prime x This is commonly written as X x2032 x03C3 X x2032 X x2032 X xA0 or xA0 X x03C3 x2032 x2032 X displaystyle left X prime sigma left X prime X right right prime X qquad text or qquad left X sigma prime right prime X This very important fact is why results for polar topologies on continuous dual spaces such as the strong dual topology x03B2 X x2032 X displaystyle beta left X prime X right on X x2032 displaystyle X prime for example can also often be applied to the original TVS X displaystyle X for instance X displaystyle X being identified with X x03C3 x2032 x2032 displaystyle left X sigma prime right prime means that the topology x03B2 X x03C3 x2032 x2032 X x03C3 x2032 displaystyle beta left left X sigma prime right prime X sigma prime right on X x03C3 x2032 x2032 displaystyle left X sigma prime right prime can instead be thought of as a topology on X displaystyle X Moreover if X x2032 displaystyle X prime is endowed with a topology that is finer than x03C3 X x2032 X displaystyle sigma left X prime X right then the continuous dual space of X x2032 displaystyle X prime will necessarily contain X x03C3 x2032 x2032 displaystyle left X sigma prime right prime as a subset So for instance when X x2032 displaystyle X prime is endowed with the strong dual topology and so is denoted by X x03B2 x2032 displaystyle X beta prime then X x03B2 x2032 x2032 xA0 x2287 xA0 X x03C3 x2032 x2032 xA0 xA0 X displaystyle left X beta prime right prime supseteq left X sigma prime right prime X which among other things allows for X displaystyle X to be endowed with the subspace topology induced on it by say the strong dual topology x03B2 X x03B2 x2032 x2032 X x03B2 x2032 displaystyle beta left left X beta prime right prime X beta prime right this topology is also called the strong bidual topology and it appears in the theory of reflexive spaces the Hausdorff locally convex TVS X displaystyle X is said to be semi reflexive if X x03B2 x2032 x2032 X displaystyle left X beta prime right prime X and it will be called reflexive if in addition the strong bidual topology x03B2 X x03B2 x2032 x2032 X x03B2 x2032 displaystyle beta left left X beta prime right prime X beta prime right on X displaystyle X is equal to X displaystyle X s original starting topology Orthogonals quotients and subspaces edit If X Y b displaystyle X Y b is a pairing then for any subset S displaystyle S of X displaystyle X S x22A5 span x2061 S x22A5 cl x03C3 Y X b x2061 span x2061 S x22A5 S x22A5 x22A5 x22A5 displaystyle S perp operatorname span S perp left operatorname cl sigma Y X b operatorname span S right perp S perp perp perp and this set is x03C3 Y X b displaystyle sigma Y X b closed 91 1 93 S x2286 S x22A5 x22A5 cl x03C3 X Y b x2061 span x2061 S displaystyle S subseteq S perp perp left operatorname cl sigma X Y b operatorname span S right 91 1 93 Thus if S displaystyle S is a x03C3 X Y b displaystyle sigma X Y b closed vector subspace of X displaystyle X then S x2286 S x22A5 x22A5 displaystyle S subseteq S perp perp If S i i x2208 I displaystyle left S i right i in I is a family of x03C3 X Y b displaystyle sigma X Y b closed vector subspaces of X displaystyle X then x22C2 i x2208 I S i x22A5 cl x03C3 Y X b x2061 span x2061 x22C3 i x2208 I S i x22A5 displaystyle left bigcap i in I S i right perp operatorname cl sigma Y X b left operatorname span left bigcup i in I S i perp right right 91 1 93 If S i i x2208 I displaystyle left S i right i in I is a family of subsets of X displaystyle X then x22C3 i x2208 I S i x22A5 x22C2 i x2208 I S i x22A5 displaystyle left bigcup i in I S i right perp bigcap i in I S i perp 91 1 93 If X displaystyle X is a normed space then under the canonical duality S x22A5 displaystyle S perp is norm closed in X x2032 displaystyle X prime and S x22A5 x22A5 displaystyle S perp perp is norm closed in X displaystyle X 91 1 93 Subspaces edit Suppose that M displaystyle M is a vector subspace of X displaystyle X and let M Y b displaystyle M Y b denote the restriction of X Y b displaystyle X Y b to M x00D7 Y displaystyle M times Y The weak topology x03C3 M Y b displaystyle sigma M Y b on M displaystyle M is identical to the subspace topology that M displaystyle M inherits from X x03C3 X Y b displaystyle X sigma X Y b Also M Y M x22A5 b M displaystyle left M Y M perp b big vert M right is a paired space where Y M x22A5 displaystyle Y M perp means Y M x22A5 displaystyle Y left M perp right where b M M x00D7 Y M x22A5 x2192 K displaystyle b big vert M M times Y M perp to mathbb K is defined by m y M x22A5 x21A6 b m y displaystyle left m y M perp right mapsto b m y The topology x03C3 M Y M x22A5 b M displaystyle sigma left M Y M perp b big vert M right is equal to the subspace topology that M displaystyle M inherits from X x03C3 X Y b displaystyle X sigma X Y b 91 5 93 Furthermore if X x03C3 X Y b displaystyle X sigma X Y b is a dual system then so is M Y M x22A5 b M displaystyle left M Y M perp b big vert M right 91 5 93 Quotients edit Suppose that M displaystyle M is a vector subspace of X displaystyle X Then X M M x22A5 b M displaystyle left X M M perp b M right is a paired space where b M X M x00D7 M x22A5 x2192 K displaystyle b M X M times M perp to mathbb K is defined by x M y x21A6 b x y displaystyle x M y mapsto b x y The topology x03C3 X M M x22A5 displaystyle sigma left X M M perp right is identical to the usual quotient topology induced by X x03C3 X Y b displaystyle X sigma X Y b on X M displaystyle X M 91 5 93 Polars and the weak topology edit If X displaystyle X is a locally convex space and if H displaystyle H is a subset of the continuous dual space X x2032 displaystyle X prime then H displaystyle H is x03C3 X x2032 X displaystyle sigma left X prime X right bounded if and only if H x2286 B x2218 displaystyle H subseteq B circ for some barrel B displaystyle B in X displaystyle X 91 1 93 The following results are important for defining polar topologies If X Y b displaystyle X Y b is a pairing and A x2286 X displaystyle A subseteq X then 91 1 93 The polar A x2218 displaystyle A circ of A displaystyle A is a closed subset of Y x03C3 Y X b displaystyle Y sigma Y X b The polars of the following sets are identical a A displaystyle A b the convex hull of A displaystyle A c the balanced hull of A displaystyle A d the x03C3 X Y b displaystyle sigma X Y b closure of A displaystyle A e the x03C3 X Y b displaystyle sigma X Y b closure of the convex balanced hull of A displaystyle A The bipolar theorem The bipolar of A displaystyle A denoted by A x2218 x2218 displaystyle A circ circ is equal to the x03C3 X Y b displaystyle sigma X Y b closure of the convex balanced hull of A displaystyle A The bipolar theorem in particular is an indispensable tool in working with dualities 91 4 93 A displaystyle A is x03C3 X Y b displaystyle sigma X Y b bounded if and only if A x2218 displaystyle A circ is absorbing in Y displaystyle Y If in addition Y displaystyle Y distinguishes points of X displaystyle X then A displaystyle A is x03C3 X Y b displaystyle sigma X Y b bounded if and only if it is x03C3 X Y b displaystyle sigma X Y b totally bounded If X Y b displaystyle X Y b is a pairing and x03C4 displaystyle tau is a locally convex topology on X displaystyle X that is consistent with duality then a subset B displaystyle B of X displaystyle X is a barrel in X x03C4 displaystyle X tau if and only if B displaystyle B is the polar of some x03C3 Y X b displaystyle sigma Y X b bounded subset of Y displaystyle Y 91 6 93 Transposes edit Transposes of a linear map with respect to pairings edit See also Transpose of a linear map Transpose and Transpose 160 Transposes of linear maps and bilinear forms Let X Y b displaystyle X Y b and W Z c displaystyle W Z c be pairings over K displaystyle mathbb K and let F X x2192 W displaystyle F X to W be a linear map For all z x2208 Z displaystyle z in Z let c F x22C5 z X x2192 K displaystyle c F cdot z X to mathbb K be the map defined by x x21A6 c F x z displaystyle x mapsto c F x z It is said that F displaystyle F 39 s transpose or adjoint is well defined if the following conditions are satisfied X displaystyle X distinguishes points of Y displaystyle Y or equivalently the map y x21A6 b x22C5 y displaystyle y mapsto b cdot y from Y displaystyle Y into the algebraic dual X x0023 displaystyle X is injective and c F x22C5 Z x2286 b x22C5 Y displaystyle c F cdot Z subseteq b cdot Y where c F x22C5 Z c F x22C5 z z x2208 Z displaystyle c F cdot Z c F cdot z z in Z and b x22C5 Y b x22C5 y y x2208 Y displaystyle b cdot Y b cdot y y in Y In this case for any span, wikipedia, wiki, book, books, library,

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