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In
mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, a bilinear form is a bilinear map on a
vector space In mathematics and physics, a vector space (also called a linear space) is a set (mathematics), set whose elements, often called vector (mathematics and physics), ''vectors'', can be added together and multiplied ("scaled") by numbers called sc ...
(the elements of which are called '' vectors'') over a field ''K'' (the elements of which are called '' scalars''). In other words, a bilinear form is a function that is
linear In mathematics, the term ''linear'' is used in two distinct senses for two different properties: * linearity of a '' function'' (or '' mapping''); * linearity of a '' polynomial''. An example of a linear function is the function defined by f(x) ...
in each argument separately: * and * and The
dot product In mathematics, the dot product or scalar productThe term ''scalar product'' means literally "product with a Scalar (mathematics), scalar as a result". It is also used for other symmetric bilinear forms, for example in a pseudo-Euclidean space. N ...
on \R^n is an example of a bilinear form which is also an
inner product In mathematics, an inner product space (or, rarely, a Hausdorff pre-Hilbert space) is a real vector space or a complex vector space with an operation called an inner product. The inner product of two vectors in the space is a scalar, ofte ...
. An example of a bilinear form that is not an inner product would be the four-vector product. The definition of a bilinear form can be extended to include modules over a ring, with
linear map In mathematics, and more specifically in linear algebra, a linear map (also called a linear mapping, linear transformation, vector space homomorphism, or in some contexts linear function) is a mapping V \to W between two vector spaces that p ...
s replaced by module homomorphisms. When is the field of
complex number In mathematics, a complex number is an element of a number system that extends the real numbers with a specific element denoted , called the imaginary unit and satisfying the equation i^= -1; every complex number can be expressed in the for ...
s , one is often more interested in sesquilinear forms, which are similar to bilinear forms but are conjugate linear in one argument.


Coordinate representation

Let be an - dimensional vector space with basis . The matrix ''A'', defined by is called the ''matrix of the bilinear form'' on the basis . If the matrix represents a vector with respect to this basis, and similarly, the matrix represents another vector , then: B(\mathbf, \mathbf) = \mathbf^\textsf A\mathbf = \sum_^n x_i A_ y_j. A bilinear form has different matrices on different bases. However, the matrices of a bilinear form on different bases are all congruent. More precisely, if is another basis of , then \mathbf_j=\sum_^n S_\mathbf_i, where the S_ form an
invertible matrix In linear algebra, an invertible matrix (''non-singular'', ''non-degenarate'' or ''regular'') is a square matrix that has an inverse. In other words, if some other matrix is multiplied by the invertible matrix, the result can be multiplied by a ...
. Then, the matrix of the bilinear form on the new basis is .


Properties


Non-degenerate bilinear forms

Every bilinear form on defines a pair of linear maps from to its
dual space In mathematics, any vector space ''V'' has a corresponding dual vector space (or just dual space for short) consisting of all linear forms on ''V,'' together with the vector space structure of pointwise addition and scalar multiplication by cons ...
. Define by This is often denoted as where the dot ( ⋅ ) indicates the slot into which the argument for the resulting
linear functional In mathematics, a linear form (also known as a linear functional, a one-form, or a covector) is a linear mapIn some texts the roles are reversed and vectors are defined as linear maps from covectors to scalars from a vector space to its field of ...
is to be placed (see Currying). For a finite-dimensional vector space , if either of or is an isomorphism, then both are, and the bilinear form is said to be nondegenerate. More concretely, for a finite-dimensional vector space, non-degenerate means that every non-zero element pairs non-trivially with some other element: :B(x,y)=0 for all y \in V implies that and :B(x,y)=0 for all x \in V implies that . The corresponding notion for a module over a commutative ring is that a bilinear form is if is an isomorphism. Given a finitely generated module over a commutative ring, the pairing may be injective (hence "nondegenerate" in the above sense) but not unimodular. For example, over the integers, the pairing is nondegenerate but not unimodular, as the induced map from to is multiplication by 2. If is finite-dimensional then one can identify with its double dual . One can then show that is the
transpose In linear algebra, the transpose of a Matrix (mathematics), matrix is an operator which flips a matrix over its diagonal; that is, it switches the row and column indices of the matrix by producing another matrix, often denoted by (among other ...
of the linear map (if is infinite-dimensional then is the transpose of restricted to the image of in ). Given one can define the ''transpose'' of to be the bilinear form given by The left radical and right radical of the form are the kernels of and respectively; they are the vectors orthogonal to the whole space on the left and on the right. If is finite-dimensional then the rank of is equal to the rank of . If this number is equal to then and are linear isomorphisms from to . In this case is nondegenerate. By the rank–nullity theorem, this is equivalent to the condition that the left and equivalently right radicals be trivial. For finite-dimensional spaces, this is often taken as the ''definition'' of nondegeneracy: Given any linear map one can obtain a bilinear form ''B'' on ''V'' via This form will be nondegenerate if and only if is an isomorphism. If is finite-dimensional then, relative to some basis for , a bilinear form is degenerate if and only if the
determinant In mathematics, the determinant is a Scalar (mathematics), scalar-valued function (mathematics), function of the entries of a square matrix. The determinant of a matrix is commonly denoted , , or . Its value characterizes some properties of the ...
of the associated matrix is zero. Likewise, a nondegenerate form is one for which the determinant of the associated matrix is non-zero (the matrix is non-singular). These statements are independent of the chosen basis. For a module over a commutative ring, a unimodular form is one for which the determinant of the associate matrix is a unit (for example 1), hence the term; note that a form whose matrix determinant is non-zero but not a unit will be nondegenerate but not unimodular, for example over the integers.


Symmetric, skew-symmetric, and alternating forms

We define a bilinear form to be * symmetric if for all , in ; * alternating if for all in ; * or if for all , in ; *; Proposition: Every alternating form is skew-symmetric. *; Proof: This can be seen by expanding . If the characteristic of is not 2 then the converse is also true: every skew-symmetric form is alternating. However, if then a skew-symmetric form is the same as a symmetric form and there exist symmetric/skew-symmetric forms that are not alternating. A bilinear form is symmetric (respectively skew-symmetric)
if and only if In logic and related fields such as mathematics and philosophy, "if and only if" (often shortened as "iff") is paraphrased by the biconditional, a logical connective between statements. The biconditional is true in two cases, where either bo ...
its coordinate matrix (relative to any basis) is symmetric (respectively skew-symmetric). A bilinear form is alternating if and only if its coordinate matrix is skew-symmetric and the diagonal entries are all zero (which follows from skew-symmetry when ). A bilinear form is symmetric if and only if the maps are equal, and skew-symmetric if and only if they are negatives of one another. If then one can decompose a bilinear form into a symmetric and a skew-symmetric part as follows B^ = \tfrac (B + ^B) \qquad B^ = \tfrac (B - ^B) , where is the transpose of (defined above).


Reflexive bilinear forms and orthogonal vectors

A bilinear form is reflexive if and only if it is either symmetric or alternating. In the absence of reflexivity we have to distinguish left and right orthogonality. In a reflexive space the left and right radicals agree and are termed the ''kernel'' or the ''radical'' of the bilinear form: the subspace of all vectors orthogonal with every other vector. A vector , with matrix representation , is in the radical of a bilinear form with matrix representation , if and only if . The radical is always a subspace of . It is trivial if and only if the matrix is nonsingular, and thus if and only if the bilinear form is nondegenerate. Suppose is a subspace. Define the '' orthogonal complement'' W^ = \left\ . For a non-degenerate form on a finite-dimensional space, the map is
bijective In mathematics, a bijection, bijective function, or one-to-one correspondence is a function between two sets such that each element of the second set (the codomain) is the image of exactly one element of the first set (the domain). Equival ...
, and the dimension of is .


Bounded and elliptic bilinear forms

Definition: A bilinear form on a normed vector space is bounded, if there is a constant such that for all , B ( \mathbf , \mathbf) \le C \left\, \mathbf \right\, \left\, \mathbf \right\, . Definition: A bilinear form on a normed vector space is elliptic, or coercive, if there is a constant such that for all , B ( \mathbf , \mathbf) \ge c \left\, \mathbf \right\, ^2 .


Associated quadratic form

For any bilinear form , there exists an associated
quadratic form In mathematics, a quadratic form is a polynomial with terms all of degree two (" form" is another name for a homogeneous polynomial). For example, 4x^2 + 2xy - 3y^2 is a quadratic form in the variables and . The coefficients usually belong t ...
defined by . When , the quadratic form ''Q'' is determined by the symmetric part of the bilinear form ''B'' and is independent of the antisymmetric part. In this case there is a one-to-one correspondence between the symmetric part of the bilinear form and the quadratic form, and it makes sense to speak of the symmetric bilinear form associated with a quadratic form. When and , this correspondence between quadratic forms and symmetric bilinear forms breaks down.


Relation to tensor products

By the
universal property In mathematics, more specifically in category theory, a universal property is a property that characterizes up to an isomorphism the result of some constructions. Thus, universal properties can be used for defining some objects independently fro ...
of the
tensor product In mathematics, the tensor product V \otimes W of two vector spaces V and W (over the same field) is a vector space to which is associated a bilinear map V\times W \rightarrow V\otimes W that maps a pair (v,w),\ v\in V, w\in W to an element of ...
, there is a canonical correspondence between bilinear forms on and linear maps . If is a bilinear form on the corresponding linear map is given by In the other direction, if is a linear map the corresponding bilinear form is given by composing ''F'' with the bilinear map that sends to . The set of all linear maps is the
dual space In mathematics, any vector space ''V'' has a corresponding dual vector space (or just dual space for short) consisting of all linear forms on ''V,'' together with the vector space structure of pointwise addition and scalar multiplication by cons ...
of , so bilinear forms may be thought of as elements of which (when is finite-dimensional) is canonically isomorphic to . Likewise, symmetric bilinear forms may be thought of as elements of (dual of the second symmetric power of ) and alternating bilinear forms as elements of (the second exterior power of ). If , .


Generalizations


Pairs of distinct vector spaces

Much of the theory is available for a bilinear mapping from two vector spaces over the same base field to that field Here we still have induced linear mappings from to , and from to . It may happen that these mappings are isomorphisms; assuming finite dimensions, if one is an isomorphism, the other must be. When this occurs, ''B'' is said to be a perfect pairing. In finite dimensions, this is equivalent to the pairing being nondegenerate (the spaces necessarily having the same dimensions). For modules (instead of vector spaces), just as how a nondegenerate form is weaker than a unimodular form, a nondegenerate pairing is a weaker notion than a perfect pairing. A pairing can be nondegenerate without being a perfect pairing, for instance via is nondegenerate, but induces multiplication by 2 on the map . Terminology varies in coverage of bilinear forms. For example, F. Reese Harvey discusses "eight types of inner product". To define them he uses diagonal matrices ''Aij'' having only +1 or −1 for non-zero elements. Some of the "inner products" are symplectic forms and some are sesquilinear forms or Hermitian forms. Rather than a general field , the instances with real numbers , complex numbers , and quaternions are spelled out. The bilinear form \sum_^p x_k y_k - \sum_^n x_k y_k is called the real symmetric case and labeled , where . Then he articulates the connection to traditional terminology:


General modules

Given a ring and a right -module and its dual module , a mapping is called a bilinear form if for all , all and all . The mapping is known as the '' natural pairing'', also called the ''canonical bilinear form'' on . A linear map induces the bilinear form , and a linear map induces the bilinear form . Conversely, a bilinear form induces the ''R''-linear maps and . Here, denotes the double dual of .


See also


Citations


References

* * * * * * * . Also: * * * * * *


External links

* * {{PlanetMath attribution, id=7553, title=Unimodular Abstract algebra Linear algebra Multilinear algebra