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Wikipedia

Linear form

In mathematics, a linear form (also known as a linear functional,[1] a one-form, or a covector) is a linear map[nb 1] from a vector space to its field of scalars (often, the real numbers or the complex numbers).

If V is a vector space over a field k, the set of all linear functionals from V to k is itself a vector space over k with addition and scalar multiplication defined pointwise. This space is called the dual space of V, or sometimes the algebraic dual space, when a topological dual space is also considered. It is often denoted Hom(V, k),[2] or, when the field k is understood, ;[3] other notations are also used, such as ,[4][5] or [2] When vectors are represented by column vectors (as is common when a basis is fixed), then linear functionals are represented as row vectors, and their values on specific vectors are given by matrix products (with the row vector on the left).

Examples edit

The constant zero function, mapping every vector to zero, is trivially a linear functional. Every other linear functional (such as the ones below) is surjective (that is, its range is all of k).

  • Indexing into a vector: The second element of a three-vector is given by the one-form   That is, the second element of   is
     
  • Mean: The mean element of an  -vector is given by the one-form   That is,
     
  • Sampling: Sampling with a kernel can be considered a one-form, where the one-form is the kernel shifted to the appropriate location.
  • Net present value of a net cash flow,   is given by the one-form   where   is the discount rate. That is,
     

Linear functionals in Rn edit

Suppose that vectors in the real coordinate space   are represented as column vectors

 

For each row vector   there is a linear functional   defined by

 
and each linear functional can be expressed in this form.

This can be interpreted as either the matrix product or the dot product of the row vector   and the column vector  :

 

Trace of a square matrix edit

The trace   of a square matrix   is the sum of all elements on its main diagonal. Matrices can be multiplied by scalars and two matrices of the same dimension can be added together; these operations make a vector space from the set of all   matrices. The trace is a linear functional on this space because   and   for all scalars   and all   matrices  

(Definite) Integration edit

Linear functionals first appeared in functional analysis, the study of vector spaces of functions. A typical example of a linear functional is integration: the linear transformation defined by the Riemann integral

 
is a linear functional from the vector space   of continuous functions on the interval   to the real numbers. The linearity of   follows from the standard facts about the integral:
 

Evaluation edit

Let   denote the vector space of real-valued polynomial functions of degree   defined on an interval   If   then let   be the evaluation functional

 
The mapping   is linear since
 

If   are   distinct points in   then the evaluation functionals     form a basis of the dual space of   (Lax (1996) proves this last fact using Lagrange interpolation).

Non-example edit

A function   having the equation of a line   with   (for example,  ) is not a linear functional on  , since it is not linear.[nb 2] It is, however, affine-linear.

Visualization edit

 
Geometric interpretation of a 1-form α as a stack of hyperplanes of constant value, each corresponding to those vectors that α maps to a given scalar value shown next to it along with the "sense" of increase. The   zero plane is through the origin.

In finite dimensions, a linear functional can be visualized in terms of its level sets, the sets of vectors which map to a given value. In three dimensions, the level sets of a linear functional are a family of mutually parallel planes; in higher dimensions, they are parallel hyperplanes. This method of visualizing linear functionals is sometimes introduced in general relativity texts, such as Gravitation by Misner, Thorne & Wheeler (1973).

Applications edit

Application to quadrature edit

If   are   distinct points in [a, b], then the linear functionals   defined above form a basis of the dual space of Pn, the space of polynomials of degree   The integration functional I is also a linear functional on Pn, and so can be expressed as a linear combination of these basis elements. In symbols, there are coefficients   for which

 
for all   This forms the foundation of the theory of numerical quadrature.[6]

In quantum mechanics edit

Linear functionals are particularly important in quantum mechanics. Quantum mechanical systems are represented by Hilbert spaces, which are antiisomorphic to their own dual spaces. A state of a quantum mechanical system can be identified with a linear functional. For more information see bra–ket notation.

Distributions edit

In the theory of generalized functions, certain kinds of generalized functions called distributions can be realized as linear functionals on spaces of test functions.

Dual vectors and bilinear forms edit

 
Linear functionals (1-forms) α, β and their sum σ and vectors u, v, w, in 3d Euclidean space. The number of (1-form) hyperplanes intersected by a vector equals the inner product.[7]

Every non-degenerate bilinear form on a finite-dimensional vector space V induces an isomorphism VV : vv such that

 

where the bilinear form on V is denoted   (for instance, in Euclidean space,   is the dot product of v and w).

The inverse isomorphism is VV : vv, where v is the unique element of V such that

 
for all  

The above defined vector vV is said to be the dual vector of  

In an infinite dimensional Hilbert space, analogous results hold by the Riesz representation theorem. There is a mapping VV from V into its continuous dual space V.

Relationship to bases edit

Basis of the dual space edit

Let the vector space V have a basis  , not necessarily orthogonal. Then the dual space   has a basis   called the dual basis defined by the special property that

 

Or, more succinctly,

 

where δ is the Kronecker delta. Here the superscripts of the basis functionals are not exponents but are instead contravariant indices.

A linear functional   belonging to the dual space   can be expressed as a linear combination of basis functionals, with coefficients ("components") ui,

 

Then, applying the functional   to a basis vector   yields

 

due to linearity of scalar multiples of functionals and pointwise linearity of sums of functionals. Then

 

So each component of a linear functional can be extracted by applying the functional to the corresponding basis vector.

The dual basis and inner product edit

When the space V carries an inner product, then it is possible to write explicitly a formula for the dual basis of a given basis. Let V have (not necessarily orthogonal) basis   In three dimensions (n = 3), the dual basis can be written explicitly

 
for   where ε is the Levi-Civita symbol and   the inner product (or dot product) on V.

In higher dimensions, this generalizes as follows

 
where   is the Hodge star operator.

Over a ring edit

Modules over a ring are generalizations of vector spaces, which removes the restriction that coefficients belong to a field. Given a module M over a ring R, a linear form on M is a linear map from M to R, where the latter is considered as a module over itself. The space of linear forms is always denoted Homk(V, k), whether k is a field or not. It is a right module, if V is a left module.

The existence of "enough" linear forms on a module is equivalent to projectivity.[8]

Dual Basis Lemma — An R-module M is projective if and only if there exists a subset   and linear forms   such that, for every   only finitely many   are nonzero, and

 

Change of field edit

Suppose that   is a vector space over   Restricting scalar multiplication to   gives rise to a real vector space[9]   called the realification of   Any vector space   over   is also a vector space over   endowed with a complex structure; that is, there exists a real vector subspace   such that we can (formally) write   as  -vector spaces.

Real versus complex linear functionals edit

Every linear functional on   is complex-valued while every linear functional on   is real-valued. If   then a linear functional on either one of   or   is non-trivial (meaning not identically  ) if and only if it is surjective (because if   then for any scalar    ), where the image of a linear functional on   is   while the image of a linear functional on   is   Consequently, the only function on   that is both a linear functional on   and a linear function on   is the trivial functional; in other words,   where   denotes the space's algebraic dual space. However, every  -linear functional on   is an  -linear operator (meaning that it is additive and homogeneous over  ), but unless it is identically   it is not an  -linear functional on   because its range (which is  ) is 2-dimensional over   Conversely, a non-zero  -linear functional has range too small to be a  -linear functional as well.

Real and imaginary parts edit

If   then denote its real part by   and its imaginary part by   Then   and   are linear functionals on   and   The fact that   for all   implies that for all  [9]

 
and consequently, that   and  [10]

The assignment   defines a bijective[10]  -linear operator   whose inverse is the map   defined by the assignment   that sends   to the linear functional   defined by

 
The real part of   is   and the bijection   is an  -linear operator, meaning that   and   for all   and  [10] Similarly for the imaginary part, the assignment   induces an  -linear bijection   whose inverse is the map   defined by sending   to the linear functional on   defined by  

This relationship was discovered by Henry Löwig in 1934 (although it is usually credited to F. Murray),[11] and can be generalized to arbitrary finite extensions of a field in the natural way. It has many important consequences, some of which will now be described.

Properties and relationships edit

Suppose   is a linear functional on   with real part   and imaginary part  

Then   if and only if   if and only if  

Assume that   is a topological vector space. Then   is continuous if and only if its real part   is continuous, if and only if  's imaginary part   is continuous. That is, either all three of   and   are continuous or none are continuous. This remains true if the word "continuous" is replaced with the word "bounded". In particular,   if and only if   where the prime denotes the space's continuous dual space.[9]

Let   If   for all scalars   of unit length (meaning  ) then[proof 1][12]

 
Similarly, if   denotes the complex part of   then   implies
 
If   is a normed space with norm   and if   is the closed unit ball then the supremums above are the operator norms (defined in the usual way) of   and   so that [12]
 
This conclusion extends to the analogous statement for polars of balanced sets in general topological vector spaces.
  • If   is a complex Hilbert space with a (complex) inner product   that is antilinear in its first coordinate (and linear in the second) then   becomes a real Hilbert space when endowed with the real part of   Explicitly, this real inner product on   is defined by   for all   and it induces the same norm on   as   because   for all vectors   Applying the Riesz representation theorem to   (resp. to  ) guarantees the existence of a unique vector   (resp.  ) such that   (resp.  ) for all vectors   The theorem also guarantees that   and   It is readily verified that   Now   and the previous equalities imply that   which is the same conclusion that was reached above.

In infinite dimensions edit

Below, all vector spaces are over either the real numbers   or the complex numbers  

If   is a topological vector space, the space of continuous linear functionals — the continuous dual — is often simply called the dual space. If   is a Banach space, then so is its (continuous) dual. To distinguish the ordinary dual space from the continuous dual space, the former is sometimes called the algebraic dual space. In finite dimensions, every linear functional is continuous, so the continuous dual is the same as the algebraic dual, but in infinite dimensions the continuous dual is a proper subspace of the algebraic dual.

A linear functional f on a (not necessarily locally convex) topological vector space X is continuous if and only if there exists a continuous seminorm p on X such that  [13]

Characterizing closed subspaces edit

Continuous linear functionals have nice properties for analysis: a linear functional is continuous if and only if its kernel is closed,[14] and a non-trivial continuous linear functional is an open map, even if the (topological) vector space is not complete.[15]

Hyperplanes and maximal subspaces edit

A vector subspace   of   is called maximal if   (meaning   and  ) and does not exist a vector subspace   of   such that   A vector subspace   of   is maximal if and only if it is the kernel of some non-trivial linear functional on   (that is,   for some linear functional   on   that is not identically 0). An affine hyperplane in   is a translate of a maximal vector subspace. By linearity, a subset   of   is a affine hyperplane if and only if there exists some non-trivial linear functional   on   such that  [11] If   is a linear functional and   is a scalar then   This equality can be used to relate different level sets of   Moreover, if   then the kernel of   can be reconstructed from the affine hyperplane   by  

Relationships between multiple linear functionals edit

Any two linear functionals with the same kernel are proportional (i.e. scalar multiples of each other). This fact can be generalized to the following theorem.

Theorem[16][17] — If   are linear functionals on X, then the following are equivalent:

  1. f can be written as a linear combination of  ; that is, there exist scalars   such that  ;
  2.  ;
  3. there exists a real number r such that   for all   and all  

If f is a non-trivial linear functional on X with kernel N,   satisfies   and U is a balanced subset of X, then   if and only if   for all  [15]

Hahn–Banach theorem edit

Any (algebraic) linear functional on a vector subspace can be extended to the whole space; for example, the evaluation functionals described above can be extended to the vector space of polynomials on all of   However, this extension cannot always be done while keeping the linear functional continuous. The Hahn–Banach family of theorems gives conditions under which this extension can be done. For example,

Hahn–Banach dominated extension theorem[18](Rudin 1991, Th. 3.2) — If   is a sublinear function, and   is a linear functional on a linear subspace   which is dominated by p on M, then there exists a linear extension   of f to the whole space X that is dominated by p, i.e., there exists a linear functional F such that

 
for all   and
 
for all  

Equicontinuity of families of linear functionals edit

Let X be a topological vector space (TVS) with continuous dual space  

For any subset H of   the following are equivalent:[19]

  1. H is equicontinuous;
  2. H is contained in the polar of some neighborhood of   in X;
  3. the (pre)polar of H is a neighborhood of   in X;

If H is an equicontinuous subset of   then the following sets are also equicontinuous: the weak-* closure, the balanced hull, the convex hull, and the convex balanced hull.[19] Moreover, Alaoglu's theorem implies that the weak-* closure of an equicontinuous subset of   is weak-* compact (and thus that every equicontinuous subset weak-* relatively compact).[20][19]

See also edit

Notes edit

Footnotes edit

  1. ^ In some texts the roles are reversed and vectors are defined as linear maps from covectors to scalars
  2. ^ For instance,  

Proofs edit

  1. ^ It is true if   so assume otherwise. Since   for all scalars   it follows that   If   then let   and   be such that   and   where if   then take  Then   and because   is a real number,   By assumption   so   Since   was arbitrary, it follows that    

References edit

  1. ^ Axler (2015) p. 101, §3.92
  2. ^ a b Tu (2011) p. 19, §3.1
  3. ^ Katznelson & Katznelson (2008) p. 37, §2.1.3
  4. ^ Axler (2015) p. 101, §3.94
  5. ^ Halmos (1974) p. 20, §13
  6. ^ Lax 1996
  7. ^ Misner, Thorne & Wheeler (1973) p. 57
  8. ^ Clark, Pete L. Commutative Algebra (PDF). Unpublished. Lemma 3.12.
  9. ^ a b c Rudin 1991, pp. 57.
  10. ^ a b c Narici & Beckenstein 2011, pp. 9–11.
  11. ^ a b Narici & Beckenstein 2011, pp. 10–11.
  12. ^ a b Narici & Beckenstein 2011, pp. 126–128.
  13. ^ Narici & Beckenstein 2011, p. 126.
  14. ^ Rudin 1991, Theorem 1.18
  15. ^ a b Narici & Beckenstein 2011, p. 128.
  16. ^ Rudin 1991, pp. 63–64.
  17. ^ Narici & Beckenstein 2011, pp. 1–18.
  18. ^ Narici & Beckenstein 2011, pp. 177–220.
  19. ^ a b c Narici & Beckenstein 2011, pp. 225–273.
  20. ^ Schaefer & Wolff 1999, Corollary 4.3.

Bibliography edit

linear, form, mathematics, linear, form, also, known, linear, functional, form, covector, linear, from, vector, space, field, scalars, often, real, numbers, complex, numbers, vector, space, over, field, linear, functionals, from, itself, vector, space, over, w. In mathematics a linear form also known as a linear functional 1 a one form or a covector is a linear map nb 1 from a vector space to its field of scalars often the real numbers or the complex numbers If V is a vector space over a field k the set of all linear functionals from V to k is itself a vector space over k with addition and scalar multiplication defined pointwise This space is called the dual space of V or sometimes the algebraic dual space when a topological dual space is also considered It is often denoted Hom V k 2 or when the field k is understood V displaystyle V 3 other notations are also used such as V displaystyle V 4 5 V displaystyle V or V displaystyle V vee 2 When vectors are represented by column vectors as is common when a basis is fixed then linear functionals are represented as row vectors and their values on specific vectors are given by matrix products with the row vector on the left Contents 1 Examples 1 1 Linear functionals in Rn 1 2 Trace of a square matrix 1 3 Definite Integration 1 4 Evaluation 1 5 Non example 2 Visualization 3 Applications 3 1 Application to quadrature 3 2 In quantum mechanics 3 3 Distributions 4 Dual vectors and bilinear forms 5 Relationship to bases 5 1 Basis of the dual space 5 2 The dual basis and inner product 6 Over a ring 7 Change of field 7 1 Real versus complex linear functionals 7 2 Real and imaginary parts 7 3 Properties and relationships 8 In infinite dimensions 8 1 Characterizing closed subspaces 8 1 1 Hyperplanes and maximal subspaces 8 1 2 Relationships between multiple linear functionals 8 2 Hahn Banach theorem 8 3 Equicontinuity of families of linear functionals 9 See also 10 Notes 10 1 Footnotes 10 2 Proofs 11 References 12 BibliographyExamples editThe constant zero function mapping every vector to zero is trivially a linear functional Every other linear functional such as the ones below is surjective that is its range is all of k Indexing into a vector The second element of a three vector is given by the one form 0 1 0 displaystyle 0 1 0 nbsp That is the second element of x y z displaystyle x y z nbsp is 0 1 0 x y z y displaystyle 0 1 0 cdot x y z y nbsp Mean The mean element of an n displaystyle n nbsp vector is given by the one form 1 n 1 n 1 n displaystyle left 1 n 1 n ldots 1 n right nbsp That is mean v 1 n 1 n 1 n v displaystyle operatorname mean v left 1 n 1 n ldots 1 n right cdot v nbsp Sampling Sampling with a kernel can be considered a one form where the one form is the kernel shifted to the appropriate location Net present value of a net cash flow R t displaystyle R t nbsp is given by the one form w t 1 i t displaystyle w t 1 i t nbsp where i displaystyle i nbsp is the discount rate That is NPV R t w R t 0 R t 1 i tdt displaystyle mathrm NPV R t langle w R rangle int t 0 infty frac R t 1 i t dt nbsp Linear functionals in Rn edit Suppose that vectors in the real coordinate space Rn displaystyle mathbb R n nbsp are represented as column vectorsx x1 xn displaystyle mathbf x begin bmatrix x 1 vdots x n end bmatrix nbsp For each row vector a a1 an displaystyle mathbf a begin bmatrix a 1 amp cdots amp a n end bmatrix nbsp there is a linear functional fa displaystyle f mathbf a nbsp defined byfa x a1x1 anxn displaystyle f mathbf a mathbf x a 1 x 1 cdots a n x n nbsp and each linear functional can be expressed in this form This can be interpreted as either the matrix product or the dot product of the row vector a displaystyle mathbf a nbsp and the column vector x displaystyle mathbf x nbsp fa x a x a1 an x1 xn displaystyle f mathbf a mathbf x mathbf a cdot mathbf x begin bmatrix a 1 amp cdots amp a n end bmatrix begin bmatrix x 1 vdots x n end bmatrix nbsp Trace of a square matrix edit The trace tr A displaystyle operatorname tr A nbsp of a square matrix A displaystyle A nbsp is the sum of all elements on its main diagonal Matrices can be multiplied by scalars and two matrices of the same dimension can be added together these operations make a vector space from the set of all n n displaystyle n times n nbsp matrices The trace is a linear functional on this space because tr sA str A displaystyle operatorname tr sA s operatorname tr A nbsp and tr A B tr A tr B displaystyle operatorname tr A B operatorname tr A operatorname tr B nbsp for all scalars s displaystyle s nbsp and all n n displaystyle n times n nbsp matrices A and B displaystyle A text and B nbsp Definite Integration edit Linear functionals first appeared in functional analysis the study of vector spaces of functions A typical example of a linear functional is integration the linear transformation defined by the Riemann integralI f abf x dx displaystyle I f int a b f x dx nbsp is a linear functional from the vector space C a b displaystyle C a b nbsp of continuous functions on the interval a b displaystyle a b nbsp to the real numbers The linearity of I displaystyle I nbsp follows from the standard facts about the integral I f g ab f x g x dx abf x dx abg x dx I f I g I af abaf x dx a abf x dx aI f displaystyle begin aligned I f g amp int a b f x g x dx int a b f x dx int a b g x dx I f I g I alpha f amp int a b alpha f x dx alpha int a b f x dx alpha I f end aligned nbsp Evaluation edit Let Pn displaystyle P n nbsp denote the vector space of real valued polynomial functions of degree n displaystyle leq n nbsp defined on an interval a b displaystyle a b nbsp If c a b displaystyle c in a b nbsp then let evc Pn R displaystyle operatorname ev c P n to mathbb R nbsp be the evaluation functionalevc f f c displaystyle operatorname ev c f f c nbsp The mapping f f c displaystyle f mapsto f c nbsp is linear since f g c f c g c af c af c displaystyle begin aligned f g c amp f c g c alpha f c amp alpha f c end aligned nbsp If x0 xn displaystyle x 0 ldots x n nbsp are n 1 displaystyle n 1 nbsp distinct points in a b displaystyle a b nbsp then the evaluation functionals evxi displaystyle operatorname ev x i nbsp i 0 n displaystyle i 0 ldots n nbsp form a basis of the dual space of Pn displaystyle P n nbsp Lax 1996 proves this last fact using Lagrange interpolation Non example edit A function f displaystyle f nbsp having the equation of a line f x a rx displaystyle f x a rx nbsp with a 0 displaystyle a neq 0 nbsp for example f x 1 2x displaystyle f x 1 2x nbsp is not a linear functional on R displaystyle mathbb R nbsp since it is not linear nb 2 It is however affine linear Visualization edit nbsp Geometric interpretation of a 1 form a as a stack of hyperplanes of constant value each corresponding to those vectors that a maps to a given scalar value shown next to it along with the sense of increase The zero plane is through the origin In finite dimensions a linear functional can be visualized in terms of its level sets the sets of vectors which map to a given value In three dimensions the level sets of a linear functional are a family of mutually parallel planes in higher dimensions they are parallel hyperplanes This method of visualizing linear functionals is sometimes introduced in general relativity texts such as Gravitation by Misner Thorne amp Wheeler 1973 Applications editApplication to quadrature edit If x0 xn displaystyle x 0 ldots x n nbsp are n 1 displaystyle n 1 nbsp distinct points in a b then the linear functionals evxi f f xi displaystyle operatorname ev x i f mapsto f left x i right nbsp defined above form a basis of the dual space of Pn the space of polynomials of degree n displaystyle leq n nbsp The integration functional I is also a linear functional on Pn and so can be expressed as a linear combination of these basis elements In symbols there are coefficients a0 an displaystyle a 0 ldots a n nbsp for whichI f a0f x0 a1f x1 anf xn displaystyle I f a 0 f x 0 a 1 f x 1 dots a n f x n nbsp for all f Pn displaystyle f in P n nbsp This forms the foundation of the theory of numerical quadrature 6 In quantum mechanics edit Linear functionals are particularly important in quantum mechanics Quantum mechanical systems are represented by Hilbert spaces which are anti isomorphic to their own dual spaces A state of a quantum mechanical system can be identified with a linear functional For more information see bra ket notation Distributions edit In the theory of generalized functions certain kinds of generalized functions called distributions can be realized as linear functionals on spaces of test functions Dual vectors and bilinear forms edit nbsp Linear functionals 1 forms a b and their sum s and vectors u v w in 3d Euclidean space The number of 1 form hyperplanes intersected by a vector equals the inner product 7 Every non degenerate bilinear form on a finite dimensional vector space V induces an isomorphism V V v v such thatv w v w w V displaystyle v w langle v w rangle quad forall w in V nbsp where the bilinear form on V is denoted displaystyle langle cdot cdot rangle nbsp for instance in Euclidean space v w v w displaystyle langle v w rangle v cdot w nbsp is the dot product of v and w The inverse isomorphism is V V v v where v is the unique element of V such that v w v w displaystyle langle v w rangle v w nbsp for all w V displaystyle w in V nbsp The above defined vector v V is said to be the dual vector of v V displaystyle v in V nbsp In an infinite dimensional Hilbert space analogous results hold by the Riesz representation theorem There is a mapping V V from V into its continuous dual space V Relationship to bases editBelow we assume that the dimension is finite For a discussion of analogous results in infinite dimensions see Schauder basis Basis of the dual space edit Let the vector space V have a basis e1 e2 en displaystyle mathbf e 1 mathbf e 2 dots mathbf e n nbsp not necessarily orthogonal Then the dual space V displaystyle V nbsp has a basis w 1 w 2 w n displaystyle tilde omega 1 tilde omega 2 dots tilde omega n nbsp called the dual basis defined by the special property thatw i ej 1if i j0if i j displaystyle tilde omega i mathbf e j begin cases 1 amp text if i j 0 amp text if i neq j end cases nbsp Or more succinctly w i ej dij displaystyle tilde omega i mathbf e j delta ij nbsp where d is the Kronecker delta Here the superscripts of the basis functionals are not exponents but are instead contravariant indices A linear functional u displaystyle tilde u nbsp belonging to the dual space V displaystyle tilde V nbsp can be expressed as a linear combination of basis functionals with coefficients components ui u i 1nuiw i displaystyle tilde u sum i 1 n u i tilde omega i nbsp Then applying the functional u displaystyle tilde u nbsp to a basis vector ej displaystyle mathbf e j nbsp yieldsu ej i 1n uiw i ej iui w i ej displaystyle tilde u mathbf e j sum i 1 n left u i tilde omega i right mathbf e j sum i u i left tilde omega i left mathbf e j right right nbsp due to linearity of scalar multiples of functionals and pointwise linearity of sums of functionals Thenu ej iui w i ej iuidij uj displaystyle begin aligned tilde u mathbf e j amp sum i u i left tilde omega i left mathbf e j right right amp sum i u i delta ij amp u j end aligned nbsp So each component of a linear functional can be extracted by applying the functional to the corresponding basis vector The dual basis and inner product edit When the space V carries an inner product then it is possible to write explicitly a formula for the dual basis of a given basis Let V have not necessarily orthogonal basis e1 en displaystyle mathbf e 1 dots mathbf e n nbsp In three dimensions n 3 the dual basis can be written explicitlyw i v 12 j 13 k 13eijk ej ek e1 e2 e3 v displaystyle tilde omega i mathbf v frac 1 2 left langle frac sum j 1 3 sum k 1 3 varepsilon ijk mathbf e j times mathbf e k mathbf e 1 cdot mathbf e 2 times mathbf e 3 mathbf v right rangle nbsp for i 1 2 3 displaystyle i 1 2 3 nbsp where e is the Levi Civita symbol and displaystyle langle cdot cdot rangle nbsp the inner product or dot product on V In higher dimensions this generalizes as followsw i v 1 i2 lt i3 lt lt in neii2 in ei2 ein e1 en v displaystyle tilde omega i mathbf v left langle frac sum 1 leq i 2 lt i 3 lt dots lt i n leq n varepsilon ii 2 dots i n star mathbf e i 2 wedge cdots wedge mathbf e i n star mathbf e 1 wedge cdots wedge mathbf e n mathbf v right rangle nbsp where displaystyle star nbsp is the Hodge star operator Over a ring editModules over a ring are generalizations of vector spaces which removes the restriction that coefficients belong to a field Given a module M over a ring R a linear form on M is a linear map from M to R where the latter is considered as a module over itself The space of linear forms is always denoted Homk V k whether k is a field or not It is a right module if V is a left module The existence of enough linear forms on a module is equivalent to projectivity 8 Dual Basis Lemma An R module M is projective if and only if there exists a subset A M displaystyle A subset M nbsp and linear forms fa a A displaystyle f a mid a in A nbsp such that for every x M displaystyle x in M nbsp only finitely many fa x displaystyle f a x nbsp are nonzero andx a Afa x a displaystyle x sum a in A f a x a nbsp Change of field editSee also Linear complex structure and Complexification Suppose that X displaystyle X nbsp is a vector space over C displaystyle mathbb C nbsp Restricting scalar multiplication to R displaystyle mathbb R nbsp gives rise to a real vector space 9 XR displaystyle X mathbb R nbsp called the realification of X displaystyle X nbsp Any vector space X displaystyle X nbsp over C displaystyle mathbb C nbsp is also a vector space over R displaystyle mathbb R nbsp endowed with a complex structure that is there exists a real vector subspace XR displaystyle X mathbb R nbsp such that we can formally write X XR XRi displaystyle X X mathbb R oplus X mathbb R i nbsp as R displaystyle mathbb R nbsp vector spaces Real versus complex linear functionals edit Every linear functional on X displaystyle X nbsp is complex valued while every linear functional on XR displaystyle X mathbb R nbsp is real valued If dim X 0 displaystyle dim X neq 0 nbsp then a linear functional on either one of X displaystyle X nbsp or XR displaystyle X mathbb R nbsp is non trivial meaning not identically 0 displaystyle 0 nbsp if and only if it is surjective because if f x 0 displaystyle varphi x neq 0 nbsp then for any scalar s displaystyle s nbsp f s f x x s displaystyle varphi left s varphi x x right s nbsp where the image of a linear functional on X displaystyle X nbsp is C displaystyle mathbb C nbsp while the image of a linear functional on XR displaystyle X mathbb R nbsp is R displaystyle mathbb R nbsp Consequently the only function on X displaystyle X nbsp that is both a linear functional on X displaystyle X nbsp and a linear function on XR displaystyle X mathbb R nbsp is the trivial functional in other words X XR 0 displaystyle X cap X mathbb R 0 nbsp where displaystyle cdot nbsp denotes the space s algebraic dual space However every C displaystyle mathbb C nbsp linear functional on X displaystyle X nbsp is an R displaystyle mathbb R nbsp linear operator meaning that it is additive and homogeneous over R displaystyle mathbb R nbsp but unless it is identically 0 displaystyle 0 nbsp it is not an R displaystyle mathbb R nbsp linear functional on X displaystyle X nbsp because its range which is C displaystyle mathbb C nbsp is 2 dimensional over R displaystyle mathbb R nbsp Conversely a non zero R displaystyle mathbb R nbsp linear functional has range too small to be a C displaystyle mathbb C nbsp linear functional as well Real and imaginary parts edit If f X displaystyle varphi in X nbsp then denote its real part by fR Re f displaystyle varphi mathbb R operatorname Re varphi nbsp and its imaginary part by fi Im f displaystyle varphi i operatorname Im varphi nbsp Then fR X R displaystyle varphi mathbb R X to mathbb R nbsp and fi X R displaystyle varphi i X to mathbb R nbsp are linear functionals on XR displaystyle X mathbb R nbsp and f fR ifi displaystyle varphi varphi mathbb R i varphi i nbsp The fact that z Re z iRe iz Im iz iIm z displaystyle z operatorname Re z i operatorname Re iz operatorname Im iz i operatorname Im z nbsp for all z C displaystyle z in mathbb C nbsp implies that for all x X displaystyle x in X nbsp 9 f x fR x ifR ix fi ix ifi x displaystyle begin alignedat 4 varphi x amp varphi mathbb R x i varphi mathbb R ix amp varphi i ix i varphi i x end alignedat nbsp and consequently that fi x fR ix displaystyle varphi i x varphi mathbb R ix nbsp and fR x fi ix displaystyle varphi mathbb R x varphi i ix nbsp 10 The assignment f fR displaystyle varphi mapsto varphi mathbb R nbsp defines a bijective 10 R displaystyle mathbb R nbsp linear operator X XR displaystyle X to X mathbb R nbsp whose inverse is the map L XR X displaystyle L bullet X mathbb R to X nbsp defined by the assignment g Lg displaystyle g mapsto L g nbsp that sends g XR R displaystyle g X mathbb R to mathbb R nbsp to the linear functional Lg X C displaystyle L g X to mathbb C nbsp defined byLg x g x ig ix for all x X displaystyle L g x g x ig ix quad text for all x in X nbsp The real part of Lg displaystyle L g nbsp is g displaystyle g nbsp and the bijection L XR X displaystyle L bullet X mathbb R to X nbsp is an R displaystyle mathbb R nbsp linear operator meaning that Lg h Lg Lh displaystyle L g h L g L h nbsp and Lrg rLg displaystyle L rg rL g nbsp for all r R displaystyle r in mathbb R nbsp and g h XR displaystyle g h in X mathbb R nbsp 10 Similarly for the imaginary part the assignment f fi displaystyle varphi mapsto varphi i nbsp induces an R displaystyle mathbb R nbsp linear bijection X XR displaystyle X to X mathbb R nbsp whose inverse is the map XR X displaystyle X mathbb R to X nbsp defined by sending I XR displaystyle I in X mathbb R nbsp to the linear functional on X displaystyle X nbsp defined by x I ix iI x displaystyle x mapsto I ix iI x nbsp This relationship was discovered by Henry Lowig in 1934 although it is usually credited to F Murray 11 and can be generalized to arbitrary finite extensions of a field in the natural way It has many important consequences some of which will now be described Properties and relationships edit Suppose f X C displaystyle varphi X to mathbb C nbsp is a linear functional on X displaystyle X nbsp with real part fR Re f displaystyle varphi mathbb R operatorname Re varphi nbsp and imaginary part fi Im f displaystyle varphi i operatorname Im varphi nbsp Then f 0 displaystyle varphi 0 nbsp if and only if fR 0 displaystyle varphi mathbb R 0 nbsp if and only if fi 0 displaystyle varphi i 0 nbsp Assume that X displaystyle X nbsp is a topological vector space Then f displaystyle varphi nbsp is continuous if and only if its real part fR displaystyle varphi mathbb R nbsp is continuous if and only if f displaystyle varphi nbsp s imaginary part fi displaystyle varphi i nbsp is continuous That is either all three of f fR displaystyle varphi varphi mathbb R nbsp and fi displaystyle varphi i nbsp are continuous or none are continuous This remains true if the word continuous is replaced with the word bounded In particular f X displaystyle varphi in X prime nbsp if and only if fR XR displaystyle varphi mathbb R in X mathbb R prime nbsp where the prime denotes the space s continuous dual space 9 Let B X displaystyle B subseteq X nbsp If uB B displaystyle uB subseteq B nbsp for all scalars u C displaystyle u in mathbb C nbsp of unit length meaning u 1 displaystyle u 1 nbsp then proof 1 12 supb B f b supb B fR b displaystyle sup b in B varphi b sup b in B left varphi mathbb R b right nbsp Similarly if fi Im f X R displaystyle varphi i operatorname Im varphi X to mathbb R nbsp denotes the complex part of f displaystyle varphi nbsp then iB B displaystyle iB subseteq B nbsp implies supb B fR b supb B fi b displaystyle sup b in B left varphi mathbb R b right sup b in B left varphi i b right nbsp If X displaystyle X nbsp is a normed space with norm displaystyle cdot nbsp and if B x X x 1 displaystyle B x in X x leq 1 nbsp is the closed unit ball then the supremums above are the operator norms defined in the usual way of f fR displaystyle varphi varphi mathbb R nbsp and fi displaystyle varphi i nbsp so that 12 f fR fi displaystyle varphi left varphi mathbb R right left varphi i right nbsp This conclusion extends to the analogous statement for polars of balanced sets in general topological vector spaces If X displaystyle X nbsp is a complex Hilbert space with a complex inner product displaystyle langle cdot cdot rangle nbsp that is antilinear in its first coordinate and linear in the second then XR displaystyle X mathbb R nbsp becomes a real Hilbert space when endowed with the real part of displaystyle langle cdot cdot rangle nbsp Explicitly this real inner product on XR displaystyle X mathbb R nbsp is defined by x y R Re x y displaystyle langle x y rangle mathbb R operatorname Re langle x y rangle nbsp for all x y X displaystyle x y in X nbsp and it induces the same norm on X displaystyle X nbsp as displaystyle langle cdot cdot rangle nbsp because x x R x x displaystyle sqrt langle x x rangle mathbb R sqrt langle x x rangle nbsp for all vectors x displaystyle x nbsp Applying the Riesz representation theorem to f X displaystyle varphi in X prime nbsp resp to fR XR displaystyle varphi mathbb R in X mathbb R prime nbsp guarantees the existence of a unique vector ff X displaystyle f varphi in X nbsp resp ffR XR displaystyle f varphi mathbb R in X mathbb R nbsp such that f x ff x displaystyle varphi x left langle f varphi x right rangle nbsp resp fR x ffR x R displaystyle varphi mathbb R x left langle f varphi mathbb R x right rangle mathbb R nbsp for all vectors x displaystyle x nbsp The theorem also guarantees that ff f X displaystyle left f varphi right varphi X prime nbsp and ffR fR XR displaystyle left f varphi mathbb R right left varphi mathbb R right X mathbb R prime nbsp It is readily verified that ff ffR displaystyle f varphi f varphi mathbb R nbsp Now ff ffR displaystyle left f varphi right left f varphi mathbb R right nbsp and the previous equalities imply that f X fR XR displaystyle varphi X prime left varphi mathbb R right X mathbb R prime nbsp which is the same conclusion that was reached above In infinite dimensions editSee also Continuous linear operatorBelow all vector spaces are over either the real numbers R displaystyle mathbb R nbsp or the complex numbers C displaystyle mathbb C nbsp If V displaystyle V nbsp is a topological vector space the space of continuous linear functionals the continuous dual is often simply called the dual space If V displaystyle V nbsp is a Banach space then so is its continuous dual To distinguish the ordinary dual space from the continuous dual space the former is sometimes called the algebraic dual space In finite dimensions every linear functional is continuous so the continuous dual is the same as the algebraic dual but in infinite dimensions the continuous dual is a proper subspace of the algebraic dual A linear functional f on a not necessarily locally convex topological vector space X is continuous if and only if there exists a continuous seminorm p on X such that f p displaystyle f leq p nbsp 13 Characterizing closed subspaces edit Continuous linear functionals have nice properties for analysis a linear functional is continuous if and only if its kernel is closed 14 and a non trivial continuous linear functional is an open map even if the topological vector space is not complete 15 Hyperplanes and maximal subspaces edit A vector subspace M displaystyle M nbsp of X displaystyle X nbsp is called maximal if M X displaystyle M subsetneq X nbsp meaning M X displaystyle M subseteq X nbsp and M X displaystyle M neq X nbsp and does not exist a vector subspace N displaystyle N nbsp of X displaystyle X nbsp such that M N X displaystyle M subsetneq N subsetneq X nbsp A vector subspace M displaystyle M nbsp of X displaystyle X nbsp is maximal if and only if it is the kernel of some non trivial linear functional on X displaystyle X nbsp that is M ker f displaystyle M ker f nbsp for some linear functional f displaystyle f nbsp on X displaystyle X nbsp that is not identically 0 An affine hyperplane in X displaystyle X nbsp is a translate of a maximal vector subspace By linearity a subset H displaystyle H nbsp of X displaystyle X nbsp is a affine hyperplane if and only if there exists some non trivial linear functional f displaystyle f nbsp on X displaystyle X nbsp such that H f 1 1 x X f x 1 displaystyle H f 1 1 x in X f x 1 nbsp 11 If f displaystyle f nbsp is a linear functional and s 0 displaystyle s neq 0 nbsp is a scalar then f 1 s s f 1 1 1sf 1 1 displaystyle f 1 s s left f 1 1 right left frac 1 s f right 1 1 nbsp This equality can be used to relate different level sets of f displaystyle f nbsp Moreover if f 0 displaystyle f neq 0 nbsp then the kernel of f displaystyle f nbsp can be reconstructed from the affine hyperplane H f 1 1 displaystyle H f 1 1 nbsp by ker f H H displaystyle ker f H H nbsp Relationships between multiple linear functionals edit Any two linear functionals with the same kernel are proportional i e scalar multiples of each other This fact can be generalized to the following theorem Theorem 16 17 If f g1 gn displaystyle f g 1 ldots g n nbsp are linear functionals on X then the following are equivalent f can be written as a linear combination of g1 gn displaystyle g 1 ldots g n nbsp that is there exist scalars s1 sn displaystyle s 1 ldots s n nbsp such that sf s1g1 sngn displaystyle sf s 1 g 1 cdots s n g n nbsp i 1nker gi ker f displaystyle bigcap i 1 n ker g i subseteq ker f nbsp there exists a real number r such that f x rgi x displaystyle f x leq rg i x nbsp for all x X displaystyle x in X nbsp and all i 1 n displaystyle i 1 ldots n nbsp If f is a non trivial linear functional on X with kernel N x X displaystyle x in X nbsp satisfies f x 1 displaystyle f x 1 nbsp and U is a balanced subset of X then N x U displaystyle N cap x U varnothing nbsp if and only if f u lt 1 displaystyle f u lt 1 nbsp for all u U displaystyle u in U nbsp 15 Hahn Banach theorem edit Main article Hahn Banach theorem Any algebraic linear functional on a vector subspace can be extended to the whole space for example the evaluation functionals described above can be extended to the vector space of polynomials on all of R displaystyle mathbb R nbsp However this extension cannot always be done while keeping the linear functional continuous The Hahn Banach family of theorems gives conditions under which this extension can be done For example Hahn Banach dominated extension theorem 18 Rudin 1991 Th 3 2 If p X R displaystyle p X to mathbb R nbsp is a sublinear function and f M R displaystyle f M to mathbb R nbsp is a linear functional on a linear subspace M X displaystyle M subseteq X nbsp which is dominated by p on M then there exists a linear extension F X R displaystyle F X to mathbb R nbsp of f to the whole space X that is dominated by p i e there exists a linear functional F such thatF m f m displaystyle F m f m nbsp for all m M displaystyle m in M nbsp and F x p x displaystyle F x leq p x nbsp for all x X displaystyle x in X nbsp Equicontinuity of families of linear functionals edit Let X be a topological vector space TVS with continuous dual space X displaystyle X nbsp For any subset H of X displaystyle X nbsp the following are equivalent 19 H is equicontinuous H is contained in the polar of some neighborhood of 0 displaystyle 0 nbsp in X the pre polar of H is a neighborhood of 0 displaystyle 0 nbsp in X If H is an equicontinuous subset of X displaystyle X nbsp then the following sets are also equicontinuous the weak closure the balanced hull the convex hull and the convex balanced hull 19 Moreover Alaoglu s theorem implies that the weak closure of an equicontinuous subset of X displaystyle X nbsp is weak compact and thus that every equicontinuous subset weak relatively compact 20 19 See also editDiscontinuous linear map Locally convex topological vector space A vector space with a topology defined by convex open sets Positive linear functional ordered vector space with a partial orderPages displaying wikidata descriptions as a fallback Multilinear form Map from multiple vectors to an underlying field of scalars linear in each argument Topological vector space Vector space with a notion of nearnessNotes editFootnotes edit In some texts the roles are reversed and vectors are defined as linear maps from covectors to scalars For instance f 1 1 a 2r 2a 2r f 1 f 1 displaystyle f 1 1 a 2r neq 2a 2r f 1 f 1 nbsp Proofs edit It is true if B displaystyle B varnothing nbsp so assume otherwise Since Re z z displaystyle left operatorname Re z right leq z nbsp for all scalars z C displaystyle z in mathbb C nbsp it follows that supx B fR x supx B f x textstyle sup x in B left varphi mathbb R x right leq sup x in B varphi x nbsp If b B displaystyle b in B nbsp then let rb 0 displaystyle r b geq 0 nbsp and ub C displaystyle u b in mathbb C nbsp be such that ub 1 displaystyle left u b right 1 nbsp and f b rbub displaystyle varphi b r b u b nbsp where if rb 0 displaystyle r b 0 nbsp then take ub 1 displaystyle u b 1 nbsp Then f b rb displaystyle varphi b r b nbsp and because f 1ubb rb textstyle varphi left frac 1 u b b right r b nbsp is a real number fR 1ubb f 1ubb rb textstyle varphi mathbb R left frac 1 u b b right varphi left frac 1 u b b right r b nbsp By assumption 1ubb B textstyle frac 1 u b b in B nbsp so f b rb supx B fR x textstyle varphi b r b leq sup x in B left varphi mathbb R x right nbsp Since b B displaystyle b in B nbsp was arbitrary it follows that supx B f x supx B fR x textstyle sup x in B varphi x leq sup x in B left varphi mathbb R x right nbsp displaystyle blacksquare nbsp References edit Axler 2015 p 101 3 92 a b Tu 2011 p 19 3 1 Katznelson amp Katznelson 2008 p 37 2 1 3 Axler 2015 p 101 3 94 Halmos 1974 p 20 13 Lax 1996 Misner Thorne amp Wheeler 1973 p 57 Clark Pete L Commutative Algebra PDF Unpublished Lemma 3 12 a b c Rudin 1991 pp 57 a b c Narici amp Beckenstein 2011 pp 9 11 a b Narici amp Beckenstein 2011 pp 10 11 a b Narici amp Beckenstein 2011 pp 126 128 Narici amp Beckenstein 2011 p 126 Rudin 1991 Theorem 1 18 a b Narici amp Beckenstein 2011 p 128 Rudin 1991 pp 63 64 Narici amp Beckenstein 2011 pp 1 18 Narici amp Beckenstein 2011 pp 177 220 a b c Narici amp Beckenstein 2011 pp 225 273 Schaefer amp Wolff 1999 Corollary 4 3 Bibliography editAxler Sheldon 2015 Linear Algebra Done Right Undergraduate Texts in Mathematics 3rd ed Springer ISBN 978 3 319 11079 0 Bishop Richard Goldberg Samuel 1980 Chapter 4 Tensor Analysis on Manifolds Dover Publications ISBN 0 486 64039 6 Conway John 1990 A course in functional analysis Graduate Texts in Mathematics Vol 96 2nd ed New York Springer Verlag ISBN 978 0 387 97245 9 OCLC 21195908 Dunford Nelson 1988 Linear operators in Romanian New York Interscience Publishers ISBN 0 471 60848 3 OCLC 18412261 Halmos Paul Richard 1974 Finite Dimensional Vector Spaces Undergraduate Texts in Mathematics 1958 2nd ed Springer ISBN 0 387 90093 4 Katznelson Yitzhak Katznelson Yonatan R 2008 A Terse Introduction to Linear Algebra American Mathematical Society ISBN 978 0 8218 4419 9 Lax Peter 1996 Linear algebra Wiley Interscience ISBN 978 0 471 11111 5 Misner Charles W Thorne Kip S Wheeler John A 1973 Gravitation W H Freeman ISBN 0 7167 0344 0 Narici Lawrence Beckenstein Edward 2011 Topological Vector Spaces Pure and applied mathematics Second ed Boca Raton FL CRC Press ISBN 978 1584888666 OCLC 144216834 Rudin Walter 1991 Functional Analysis International Series in Pure and Applied Mathematics Vol 8 Second ed New York NY McGraw Hill Science Engineering Math ISBN 978 0 07 054236 5 OCLC 21163277 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 Schutz Bernard 1985 Chapter 3 A first course in general relativity Cambridge UK Cambridge University Press ISBN 0 521 27703 5 Treves Francois 2006 1967 Topological Vector Spaces Distributions and Kernels Mineola N Y Dover Publications ISBN 978 0 486 45352 1 OCLC 853623322 Tu Loring W 2011 An Introduction to Manifolds Universitext 2nd ed Springer ISBN 978 0 8218 4419 9 Wilansky Albert 2013 Modern Methods in Topological Vector Spaces Mineola New York Dover Publications Inc ISBN 978 0 486 49353 4 OCLC 849801114 Retrieved from https en wikipedia org w index php title Linear form amp oldid 1206557204, wikipedia, wiki, book, books, library,

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