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Contents

   



(Top)
 


1 Coordinate representation  





2 Properties  



2.1  Non-degenerate bilinear forms  





2.2  Symmetric, skew-symmetric, and alternating forms  





2.3  Reflexive bilinear forms and orthogonal vectors  





2.4  Bounded and elliptic bilinear forms  







3 Associated quadratic form  





4 Relation to tensor products  





5 Generalizations  



5.1  Pairs of distinct vector spaces  





5.2  General modules  







6 See also  





7 Citations  





8 References  





9 External links  














Bilinear form






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From Wikipedia, the free encyclopedia
 


Inmathematics, a bilinear form is a bilinear map V × VK on a vector space V (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 B : V × VK that is linear in each argument separately:

The dot producton is an example of a bilinear form.[1]

The definition of a bilinear form can be extended to include modules over a ring, with linear maps replaced by module homomorphisms.

When K is the field of complex numbers C, one is often more interested in sesquilinear forms, which are similar to bilinear forms but are conjugate linear in one argument.

Coordinate representation[edit]

Let V be an n-dimensional vector space with basis {e1, …, en}.

The n × n matrix A, defined by Aij = B(ei, ej) is called the matrix of the bilinear form on the basis {e1, …, en}.

If the n × 1 matrix x represents a vector x with respect to this basis, and similarly, the n × 1 matrix y represents another vector y, then:

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 {f1, …, fn} is another basis of V, then

where the form an invertible matrix S. Then, the matrix of the bilinear form on the new basis is STAS.

Properties[edit]

Non-degenerate bilinear forms[edit]

Every bilinear form BonV defines a pair of linear maps from V to its dual space V. Define B1, B2: VVby

B1(v)(w) = B(v, w)
B2(v)(w) = B(w, v)

This is often denoted as

B1(v) = B(v, ⋅)
B2(v) = B(⋅, v)

where the dot ( ⋅ ) indicates the slot into which the argument for the resulting linear functional is to be placed (see Currying).

For a finite-dimensional vector space V, if either of B1orB2 is an isomorphism, then both are, and the bilinear form B 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:

for all implies that x = 0 and
for all implies that y = 0.

The corresponding notion for a module over a commutative ring is that a bilinear form is unimodularifVV 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 B(x, y) = 2xy is nondegenerate but not unimodular, as the induced map from V = ZtoV = Z is multiplication by 2.

IfV is finite-dimensional then one can identify V with its double dual V∗∗. One can then show that B2 is the transpose of the linear map B1 (ifV is infinite-dimensional then B2 is the transpose of B1 restricted to the image of VinV∗∗). Given B one can define the transposeofB to be the bilinear form given by

tB(v, w) = B(w, v).

The left radical and right radical of the form B are the kernelsofB1 and B2 respectively;[2] they are the vectors orthogonal to the whole space on the left and on the right.[3]

IfV is finite-dimensional then the rankofB1 is equal to the rank of B2. If this number is equal to dim(V) then B1 and B2 are linear isomorphisms from VtoV. In this case B 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:

Definition: BisnondegenerateifB(v, w) = 0 for all w implies v = 0.

Given any linear map A : VV one can obtain a bilinear form BonV via

B(v, w) = A(v)(w).

This form will be nondegenerate if and only if A is an isomorphism.

IfVisfinite-dimensional then, relative to some basis for V, a bilinear form is degenerate if and only if the determinant 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 B(x, y) = 2xy over the integers.

Symmetric, skew-symmetric, and alternating forms[edit]

We define a bilinear form to be

If the characteristicofK is not 2 then the converse is also true: every skew-symmetric form is alternating. However, if char(K) = 2 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 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 char(K) ≠ 2).

A bilinear form is symmetric if and only if the maps B1, B2: VV are equal, and skew-symmetric if and only if they are negatives of one another. If char(K) ≠ 2 then one can decompose a bilinear form into a symmetric and a skew-symmetric part as follows

where tB is the transpose of B (defined above).

Reflexive bilinear forms and orthogonal vectors[edit]

Definition: A bilinear form B : V × VK is called reflexiveifB(v, w) = 0 implies B(w, v) = 0 for all v, winV.
Definition: Let B : V × VK be a reflexive bilinear form. v, winV are orthogonal with respect to BifB(v, w) = 0.

A bilinear form B is reflexive if and only if it is either symmetric or alternating.[4] 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 v, with matrix representation x, is in the radical of a bilinear form with matrix representation A, if and only if Ax = 0 ⇔ xTA = 0. The radical is always a subspace of V. It is trivial if and only if the matrix A is nonsingular, and thus if and only if the bilinear form is nondegenerate.

Suppose W is a subspace. Define the orthogonal complement[5]

For a non-degenerate form on a finite-dimensional space, the map V/WWisbijective, and the dimension of Wisdim(V) − dim(W).

Bounded and elliptic bilinear forms[edit]

Definition: A bilinear form on a normed vector space (V, ‖⋅‖)isbounded, if there is a constant C such that for all u, vV,

Definition: A bilinear form on a normed vector space (V, ‖⋅‖)iselliptic, or coercive, if there is a constant c > 0 such that for all uV,

Associated quadratic form[edit]

For any bilinear form B : V × VK, there exists an associated quadratic form Q : VK defined by Q : VK : vB(v, v).

When char(K) ≠ 2, 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 char(K) = 2 and dim V >1, this correspondence between quadratic forms and symmetric bilinear forms breaks down.

Relation to tensor products[edit]

By the universal property of the tensor product, there is a canonical correspondence between bilinear forms on V and linear maps VVK. If B is a bilinear form on V the corresponding linear map is given by

vwB(v, w)

In the other direction, if F : VVK is a linear map the corresponding bilinear form is given by composing F with the bilinear map V × VVV that sends (v, w)tovw.

The set of all linear maps VVK is the dual spaceofVV, so bilinear forms may be thought of as elements of (VV) which (when V is finite-dimensional) is canonically isomorphic to VV.

Likewise, symmetric bilinear forms may be thought of as elements of (Sym2V)* (dual of the second symmetric powerofV) and alternating bilinear forms as elements of 2V) ≃ Λ2V (the second exterior powerofV). If charK ≠ 2, (Sym2V)* ≃ Sym2(V).

Generalizations[edit]

Pairs of distinct vector spaces[edit]

Much of the theory is available for a bilinear mapping from two vector spaces over the same base field to that field

B : V × WK.

Here we still have induced linear mappings from VtoW, and from WtoV. 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 Z × ZZ via (x, y) ↦ 2xy is nondegenerate, but induces multiplication by 2 on the map ZZ.

Terminology varies in coverage of bilinear forms. For example, F. Reese Harvey discusses "eight types of inner product".[6] 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 formsorHermitian forms. Rather than a general field K, the instances with real numbers R, complex numbers C, and quaternions H are spelled out. The bilinear form

is called the real symmetric case and labeled R(p, q), where p + q = n. Then he articulates the connection to traditional terminology:[7]

Some of the real symmetric cases are very important. The positive definite case R(n, 0) is called Euclidean space, while the case of a single minus, R(n−1, 1) is called Lorentzian space. If n = 4, then Lorentzian space is also called Minkowski spaceorMinkowski spacetime. The special case R(p, p) will be referred to as the split-case.

General modules[edit]

Given a ring R and a right R-module M and its dual module M, a mapping B : M × MR is called a bilinear formif

B(u + v, x) = B(u, x) + B(v, x)
B(u, x + y) = B(u, x) + B(u, y)
B(αu, ) = αB(u, x)β

for all u, vM, all x, yM and all α, βR.

The mapping ⟨⋅,⋅⟩ : M × MR : (u, x) ↦ u(x) is known as the natural pairing, also called the canonical bilinear formonM × M.[8]

A linear map S : MM : uS(u) induces the bilinear form B : M × MR : (u, x) ↦ ⟨S(u), x, and a linear map T : MM : xT(x) induces the bilinear form B : M × MR : (u, x) ↦ ⟨u, T(x)⟩.

Conversely, a bilinear form B : M × MR induces the R-linear maps S : MM : u ↦ (xB(u, x)) and T′ : MM∗∗ : x ↦ (uB(u, x)). Here, M∗∗ denotes the double dualofM.

See also[edit]

  • Category:Bilinear maps
  • Inner product space
  • Linear form
  • Multilinear form
  • Polar space
  • Quadratic form
  • Sesquilinear form
  • System of bilinear equations
  • Citations[edit]

    1. ^ "Chapter 3. Bilinear forms — Lecture notes for MA1212" (PDF). 2021-01-16.
  • ^ Jacobson 2009, p. 346.
  • ^ Zhelobenko 2006, p. 11.
  • ^ Grove 1997.
  • ^ Adkins & Weintraub 1992, p. 359.
  • ^ Harvey 1990, p. 22.
  • ^ Harvey 1990, p. 23.
  • ^ Bourbaki 1970, p. 233.
  • References[edit]

    External links[edit]

    This article incorporates material from Unimodular on PlanetMath, which is licensed under the Creative Commons Attribution/Share-Alike License.


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