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In mathematics, the tensor product VW of two vector spaces V and W (over the same field) is itself a vector space, endowed with the operation of bilinear composition, denoted by , from ordered pairs in the Cartesian product V × W onto VW in a way that generalizes the outer product.

Essentially the difference between a tensor product of two vectors and an ordered pair of vectors is that if one vector is multiplied by a nonzero scalar and the other is multiplied by the reciprocal of that scalar, the result is a different ordered pair of vectors, but the same tensor product of two vectors.

The tensor product of V and W is the vector space generated by the symbols vw, with vV and wW, in which the relations of bilinearity are imposed for the product operation , and no other relations are assumed to hold. The tensor product space is thus the "freest" (or most general) such vector space, in the sense of having the fewest constraints.

The tensor product of (finite-dimensional) vector spaces has dimension equal to the product of the dimensions of the two factors:

In particular, this distinguishes the tensor product from the direct sum vector space, whose dimension is the sum of the dimensions of the two summands:

More generally, the tensor product can be extended to other categories of mathematical objects in addition to vector spaces, such as to matrices, tensors, algebras, topological vector spaces, and modules. In each such case the tensor product is characterized by a similar universal property: it is the freest bilinear operation. The general concept of a "tensor product" is captured by monoidal categories; that is, the class of all things that have a tensor product is a monoidal category.

Intuitive motivation and the concrete tensor productEdit

The intuitive motivation for the tensor product relies on the concept of tensors more generally. In particular, a tensor is an object which can be considered a special type of multilinear map, which takes in a certain number of vectors (its order) and outputs a scalar. Such objects are useful in a number of areas of application, such as Riemannian geometry, famous for its use in Albert Einstein's general theory of relativity in modern physics, where the metric tensor is a fundamental concept: in particular, the metric tensor takes in two vectors, conceived of roughly as small arrows emanating from a specific point within a curved space, or manifold, and returns a local dot product of them relative to that particular point—an operation which encodes roughly the vectors' lengths as well as the angle between them. As the dot product is a scalar, the metric tensor is thus seen to deserve its name. There is one metric tensor at each point of the manifold, and variation in the metric tensor thus encodes how that distance and angle concepts, and so the laws of analytic geometry, vary throughout the manifold.

One can think of the tensor product of two vector spaces,   and   as representing the set of all tensors that take a vector from   and   and output a scalar within their common base field (and thus can only be defined if they have such a base field). The two spaces may be the same—in the above they are vectors in the tangent space at a point: roughly the flat space a tiny piece of the manifold most "looks like" when you zoom very, very close into a particular point therein, and thus the metric tensor lives in the tensor product of that space with itself. But they may also be different.

If we have a basis for the vector spaces, and the vector space is finite-dimensional, we can represent the vectors in terms of components under those basis vectors:

 

where each notation stands for the sum  .

A tensor is then a map   that works as above, returning a scalar and is linear in both of its arguments. Such a tensor can be represented using a matrix multiplication:

 

where the superscripted T denotes the matrix transpose which sends the vector   to its dual vector.

Given two vectors, we can form a tensor of their own from them rather naturally using the outer product, which is denoted   and equals  . This tensor comes out as the matrix

 

and this matrix corresponds to the tensor by the prior construction, which is reminiscent of how it corresponds to a linear map (by multiplying on one side only). These tensors themselves generate a vector space by adding them together and multiplying them by scalars in the usual ways that we do for matrices and functions, and the collection of all such tensors so formed is the tensor product   of the two vector spaces themselves. In fact, this space is equivalent to the space of maps represented by every possible matrix of the above size, as can be seen by noting that the simple tensor products   (here   is the basis of the other vector space,  ) have a "1" in the  -th position and "0"s everywhere else, which allows them to be multiplied by any number and then added up to get a matrix with arbitrary entries.

The purpose of the succeeding sections is to find a definition that is equivalent to this where it is applicable but which does not require a specific choice of basis and which can also more easily be applied to infinite-dimensional settings where the usual basis concepts (Hamel basis) may be ill-behaved. Not requiring a specific basis is useful from a theoretical point of view since while every vector space has a basis, not all bases are necessarily constructible, and moreover that result itself depends on the acceptance of the axiom of choice which may be rejected in some systems of mathematics. Also, it is useful to find an abstract construction for analysis from the point of view of category theory, the theory of the very zoomed-out "big picture of maths" and how all mathematical objects relate to each other in a very general sense. A very important real-life use for having such a definition can be found in another field of modern physics called quantum mechanics: the tensor product in this form allows us to talk of the wave function of a system of two particles as an abstract Hilbert space vector without having to specify a specific basis of observables.

Baby step towards the abstract tensor product: the free vector spaceEdit

The first step we will consider involves introducing something which is called a "free vector space" over a given set. The thrust behind this idea basically consists of what we said in the last point: since a tensor   can be written by the double sum

 

the most natural way to approach this problem is somehow to figure out how we can "forget" about the specific choice of bases   and   that are used here. In mathematics, the way we "forget" about representational details of something is to establish an identification that tells us that two different things which are to be considered representations of the same thing are in fact such, i.e. which, given those says either "yes, they are" or "no, they aren't", and then "lump together" all representations as constituting the "thing represented" without reference to any one in particular by packaging them all together into a single set. In formal terms, we first build an equivalence relation, and then take the quotient set by that relation.

But before we can do that, we first need to develop what we are going to take the equivalence relation over. The way we do that is to approach this the other way around, from the "bottom up": since we are not guaranteed a, at least constructible, basis when starting from arbitrary vector spaces, we might instead try to start by guaranteeing we have one—that is, we will start first by considering a "basis", on its own, as given, and then building the vector space on top. To that end, we accomplish the following: suppose that   is some set, which we could call an abstract basis set. Now consider all formal expressions of the form

 

of arbitrary, but finite, length   and for which   are scalars and   are members of  . Intuitively, this is a linear combination of the basis vectors in the usual sense of expanding an element of a vector space. We call this a "formal expression" because technically it is illegal to multiply   since there is no defined multiplication operation by default on an arbitrary set and arbitrary field of scalars. Instead, we will "pretend" (similar to defining the imaginary numbers) that this refers to something, and then will go about manipulating it according to the rules we expect for a vector space, e.g. the sum of two such strings of the same length is

 

where we have used the associative, commutative, and distributive laws to rearrange the first sum into the second. Continuing this way for scalar multiples and all different-length combinations of vectors allows us to build up a vector addition and scalar multiplication on this set of formal expressions, and we call it the free vector space over  , writing  . Note that the elements of  , considered as length-one formal expressions with coefficient 1 out front, form a Hamel basis for this space.

The tensor product expression is then abstracted by considering that if   and   represent "abstract basis vectors" from two sets   and  , i.e. that " " and " ", then pairs of these in the Cartesian product  , i.e.   are taken as standing for the tensor products  . (Note that the tensor products in the expression are in some sense "atomic", i.e. additions and scalar multiplications do not split them up into anything else, so we can replace them with something different without altering the mathematical structure.) With such an identification, we can thus define the tensor product of two free vector spaces   and   as being something (yet to be decided) which is isomorphic to  .

Using the free vector space to "forget" about the basisEdit

The above definition will actually work for any vector space in which we can specify a basis, since we can just rebuild it as the free vector space over that basis: the above construction exactly mirrors how you represent vectors via the Hamel basis construction by design. In effect, we haven't gained anything ... until we do this.

Since we are assuming we don't actually have access to a basis for each vector space   and   that we in general want to form the tensor product   of, we will instead do the next best thing and in some sense the one thing we are guaranteed able to do, regardless of any concerns or problematics in finding a specific basis: take all of   and   as "basis" to build up the tensors—which corresponds to actually what we did in the last part of the "Intuitive motivation" section where we considered adding together arbitrary outer products   of arbitrary vectors taken from the two spaces. The only difference here is that if we use the free vector space construction and form the obvious   it will have many redundant versions of what should be the same tensor, i.e. going back to our basisful case if we consider the very specific example where   in the standard basis, which is manageably small yet nontrivial, we may consider that the tensor formed by the vectors   and  , i.e.

 

could also be represented by other sums, such as the sum using individual basic tensors  , e.g.

 

These, while equal expressions in the concrete case, would correspond to distinct elements of the free vector space  , namely

 

in the first case and

 

in the second case. Thus we must condense them—this is where the equivalence relation comes into play. The trick to building it is to note that given any vector   in a vector space, it is always possible to represent it as the sum of two other vectors   and   not equal to the original. If nothing else, let   be any vector and then take  —which also shows that if we are given one vector and then a second vector, we can write the first vector in terms of the second together with a suitable third vector (indeed in many ways—just consider scalar multiples of the second vector in the same subtraction.).

This is useful to us because the outer product satisfies the following linearity properties, which can be proven by simple algebra on the corresponding matrix expressions (the vectors below are generic, not the example ones above):

 
 
 
 

If we want to relate the outer product   to, say,  , we can use the first relation above together with a suitable expression of   as a sum of some vector and some scalar multiple of  .

Equality between two concrete tensors is then obtained if using the above rules will permit us to rearrange one sum of outer products into the other by suitably decomposing vectors—regardless of if we have a set of actual basis vectors. Applying that to our example above, we see that of course we have

 
 

for which substitution in

 

gives us

 

and judicious use of the distributivity properties lets us rearrange to the desired form. Likewise, there is a corresponding "mirror" manipulation in terms of the free vector space elements   and  ,  , etc, and this finally leads us to the formal definition of the tensor product.

The definition of the abstract tensor productEdit

The abstract tensor product of two vector spaces   and   over a common base field is the quotient vector space

 

where   is the equivalence relation of formal equality which is generated by assuming that for each   and   taken as formal expressions in the free vector space the following hold:

Identity.  
Distributivity.   and  
Scalar multiples.   and  

and then testing equivalence of generic formal expressions through suitable manipulations based thereupon.[citation needed] Arithmetic is defined on the tensor product by choosing representative elements, applying the arithmetical rules, and finally taking the equivalence class. Moreover, given any two vectors   and  , the equivalence class   is denoted  .

PropertiesEdit

NotationEdit

Elements of VW are often referred to as tensors, although this term refers to many other related concepts as well.[1] If v belongs to V and w belongs to W, then the equivalence class of (v, w) is denoted by vw, which is called the tensor product of v with w. In physics and engineering, this use of the "⊗" symbol refers specifically to the outer product operation; the result of the outer product vw is one of the standard ways of representing the equivalence class vw.[2] An element of VW that can be written in the form vw is called a pure or simple tensor. In general, an element of the tensor product space is not a pure tensor, but rather a finite linear combination of pure tensors. For example, if v1 and v2 are linearly independent, and w1 and w2 are also linearly independent, then v1w1 + v2w2 cannot be written as a pure tensor. The number of simple tensors required to express an element of a tensor product is called the tensor rank (not to be confused with tensor order, which is the number of spaces one has taken the product of, in this case 2; in notation, the number of indices), and for linear operators or matrices, thought of as (1, 1) tensors (elements of the space VV), it agrees with matrix rank.

DimensionEdit

Given bases {vi} and {wj} for V and W respectively, the tensors {viwj} form a basis for VW. Therefore, if V and W are finite-dimensional, the dimension of the tensor product is the product of dimensions of the original spaces; for instance RmRn is isomorphic to Rmn.

Tensor product of linear mapsEdit

The tensor product also operates on linear maps between vector spaces. Specifically, given two linear maps S : VX and T : WY between vector spaces, the tensor product of the two linear maps S and T is a linear map

 

defined by

 

In this way, the tensor product becomes a bifunctor from the category of vector spaces to itself, covariant in both arguments.[3]

If S and T are both injective, surjective, or continuous then ST is, respectively, injective, surjective, continuous.

By choosing bases of all vector spaces involved, the linear maps S and T can be represented by matrices. Then, the matrix describing the tensor product ST is the Kronecker product of the two matrices. For example, if V, X, W, and Y above are all two-dimensional and bases have been fixed for all of them, and S and T are given by the matrices

 

respectively, then the tensor product of these two matrices is

 

The resultant rank is at most 4, and thus the resultant dimension is 4. Note that rank here denotes the tensor rank i.e. the number of requisite indices (while the matrix rank counts the number of degrees of freedom in the resulting array).

A dyadic product is the special case of the tensor product between two vectors of the same dimension.

Universal propertyEdit

 
This commutative diagram presents the universal property of tensor product. Here   and   are bilinear, whereas   is linear.

In the context of vector spaces, the tensor product   and the associated bilinear map   are characterized up to isomorphism by a universal property regarding bilinear maps. (Recall that a bilinear map is a function that is separately linear in each of its arguments.) Informally,   is the most general bilinear map out of  .

The vector space   and the associated bilinear map   have the property that any bilinear map   from   to any vector space   factors through   uniquely. By saying "  factors through   uniquely," we mean that there is a unique linear map   such that  .

This characterization can simplify proofs about the tensor product. For example, the tensor product is symmetric, meaning there is a canonical isomorphism:

 

To construct, say, a map from   to  , it suffices to give a bilinear map   that maps   to  . Then the universal property of   means   factors into a map  . A map   in the opposite direction is similarly defined, and one checks that the two linear maps   and   are inverse to one another by again using their universal properties.

Similar reasoning can be used to show that the tensor product is associative, that is, there are natural isomorphisms

 

Therefore, it is customary to omit the parentheses and write  .

The category of vector spaces with tensor product is an example of a symmetric monoidal category.

The universal-property definition of a tensor product is valid in more categories than just the category of vector spaces. Instead of using multilinear (bilinear) maps, the general tensor product definition uses multimorphisms.[4]

Tensor powers and braidingEdit

Let n be a non-negative integer. The nth tensor power of the vector space V is the n-fold tensor product of V with itself. That is

 

A permutation σ of the set {1, 2, ..., n} determines a mapping of the nth Cartesian power of V as follows:

 

Let

 

be the natural multilinear embedding of the Cartesian power of V into the tensor power of V. Then, by the universal property, there is a unique isomorphism

 

such that

 

The isomorphism τσ is called the braiding map associated to the permutation σ.

Product of tensorsEdit

For non-negative integers r and s a type (r,s) tensor on a vector space V is an element of

 

Here V is the dual vector space (which consists of all linear maps f from V to the ground field K).

There is a product map, called the (tensor) product of tensors[5]

 

It is defined by grouping all occurring "factors" V together: writing vi for an element of V and fi for elements of the dual space,

 

Picking a basis of V and the corresponding dual basis of V naturally induces a basis for Tr
s
(V)
(this basis is described in the article on Kronecker products). In terms of these bases, the components of a (tensor) product of two (or more) tensors can be computed. For example, if F and G are two covariant tensors of rank m and n respectively (i.e. FT 0
m
, and GT 0
n
), then the components of their tensor product are given by

 

[6] Thus, the components of the tensor product of two tensors are the ordinary product of the components of each tensor. Another example: let U be a tensor of type (1, 1) with components Uαβ, and let V be a tensor of type (1, 0) with components Vγ. Then

 

and

 

Products of tensors form an algebra, called the tensor algebra.

Relation to dual spaceEdit

A particular example is the tensor product of some vector space V with its dual vector space V (which consists of all linear maps f from V to the ground field K). In this case, there is a canonical evaluation map

 

which on elementary tensors is defined by

 

The resulting map

 

is called tensor contraction (for r, s > 0).

On the other hand, if V is finite-dimensional, there is a canonical map in the other direction (called the coevaluation map)

 

where v1, ..., vn is any basis of V, and vi is its dual basis. Surprisingly, this map does not depend on our choice of basis.[7]

The interplay of evaluation and coevaluation map can be used to characterize finite-dimensional vector spaces without referring to bases.[8]

Tensor product vs. HomEdit

Given two finite dimensional vector spaces U, V over the same field K, denote the dual space of U as U*, and K-vector space of all linear maps from U to V as Hom(U,V). We have the following relation:

 

an isomorphism can be defined by  , when acting on pure tensors

 

its "inverse" can be defined in a similar manner as above (Relation to dual space) using dual basis  ,

 

This result implies

 

which automatically gives the important fact that   forms a basis for   where   are bases of U and V.

Furthermore, given three vector spaces U, V, W the tensor product is linked to the vector space of all linear maps, as follows:

 

This is an example of adjoint functors: the tensor product is "left adjoint" to Hom.

Adjoint representationEdit

The tensor   may be naturally viewed as a module for the Lie algebra End(V) by means of the diagonal action: for simplicity let us assume r = s = 1, then, for each u ∈ End(V),

 

where u in End(V) is the transpose of u, that is, in terms of the obvious pairing on VV,

 .

There is a canonical isomorphism   given by

 

Under this isomorphism, every u in End(V) may be first viewed as an endomorphism of   and then viewed as an endomorphism of End(V). In fact it is the adjoint representation ad(u) of End(V).

Tensor products of modules over a ringEdit

The tensor product of two modules A and B over a commutative ring R is defined in exactly the same way as the tensor product of vector spaces over a field:

 

where now F(A × B) is the free R-module generated by the cartesian product and G is the R-module generated by the same relations as above.

More generally, the tensor product can be defined even if the ring is non-commutative (abba). In this case A has to be a right-R-module and B is a left-R-module, and instead of the last two relations above, the relation

 

is imposed. If R is non-commutative, this is no longer an R-module, but just an abelian group.

The universal property also carries over, slightly modified: the map φ : A × BAR B defined by (a, b) ↦ ab is a middle linear map (referred to as "the canonical middle linear map".[9]); that is,[10] it satisfies:

 

The first two properties make φ a bilinear map of the abelian group A × B. For any middle linear map ψ of A × B, a unique group homomorphism f of AR B satisfies ψ = fφ, and this property determines   within group isomorphism. See the main article for details.

Tensor product of modules over a non-commutative ringEdit

Let A be a right R-module and B be a left R-module B. Then the tensor product of A and B is an abelian group defined by

 

where   is a free abelian group over   and G is a subgroup of   generated by relations

 

The universal property can be stated as follows. Let G be an abelian group with a map   which is bilinear, in the sense that

 

Then there is a unique map   such that   for every  .

Furthermore, we can give   a module structure under some extra conditions.

1) If A was a (S,R)-bimodule, then   is a left S-module where  .
2) If B was a (R,S)-bimodule, then   is a right S-module where  .
3) If R was a commutative ring, then A and B are (R,R)-bimodules where   and  . By 1),   is a left R-module. By 2),   is a right R-module. So we can conclude   is a (R,R)-bimodule.

Computing the tensor productEdit

For vector spaces, the tensor product VW is quickly computed since bases of V of W immediately determine a basis of VW, as was mentioned above. For modules over a general (commutative) ring, not every module is free. For example, Z/nZ is not a free abelian group (= Z-module). The tensor product with Z/nZ is given by

 

More generally, given a presentation of some R-module M, that is, a number of generators miM, iI together with relations

 

the tensor product can be computed as the following cokernel:

 

Here NJ := ⨁jJ N and the map is determined by sending some nN in the jth copy of NJ to ajin (in NI). Colloquially, this may be rephrased by saying that a presentation of M gives rise to a presentation of MR N. This is referred to by saying that the tensor product is a right exact functor. It is not in general left exact, that is, given an injective map of R-modules M1M2, the tensor product

 

is not usually injective. For example, tensoring the (injective) map given by multiplication with n, n : ZZ with Z/nZ yields the zero map 0 : Z/nZZ/nZ, which is not injective. Higher Tor functors measure the defect of the tensor product being not left exact. All higher Tor functors are assembled in the derived tensor product.

Tensor product of algebrasEdit

Let R be a commutative ring. The tensor product of R-modules applies, in particular, if A and B are R-algebras. In this case, the tensor product AR B is an R-algebra itself by putting

 

For example,

 

A particular example is when A and B are fields containing a common subfield R. The tensor product of fields is closely related to Galois theory: if, say, A = R[x] / f(x), where f is some irreducible polynomial with coefficients in R, the tensor product can be calculated as

 

where now f is interpreted as the same polynomial, but with its coefficients regarded as elements of B. In the larger field B, the polynomial may become reducible, which brings in Galois theory. For example, if A = B is a Galois extension of R, then

 

is isomorphic (as an A-algebra) to the Adeg(f).

Eigenconfigurations of tensorsEdit

Square matrices A with entries in a field K represent linear maps of vector spaces, say  , and thus linear maps   of projective spaces over  . If A is nonsingular then   is well-defined everywhere, and the eigenvectors of   correspond to the fixed points of  . The eigenconfiguration of A consists of   points in  , provided   is generic and K is algebraically closed. The fixed points of nonlinear maps are the eigenvectors of tensors. Let   be a  -dimensional tensor of format   with entries   lying in an algebraically closed field   of characteristic zero. Such a tensor   defines polynomial maps   and   with coordinates

 

Thus each of the   coordinates of   is a homogeneous polynomial   of degree   in  . The eigenvectors of   are the solutions of the constraint

 

and the eigenconfiguration is given by the variety of the   minors of this matrix.[11]

Other examples of tensor productsEdit

Tensor product of Hilbert spacesEdit

Hilbert spaces generalize finite-dimensional vector spaces to countably-infinite dimensions. The tensor product is still defined; it is the tensor product of Hilbert spaces.

Topological tensor productEdit

When the basis for a vector space is no longer countable, then the appropriate axiomatic formalization for the vector space is that of a topological vector space. The tensor product is still defined, it is the topological tensor product.

Tensor product of graded vector spacesEdit

Some vector spaces can be decomposed into direct sums of subspaces. In such cases, the tensor product of two spaces can be decomposed into sums of products of the subspaces (in analogy to the way that multiplication distributes over addition).

Tensor product of representationsEdit

Vector spaces endowed with an additional multiplicative structure are called algebras. The tensor product of such algebras is described by the Littlewood–Richardson rule.

Tensor product of quadratic formsEdit

Tensor product of multilinear formsEdit

Given two multilinear forms   and   on a vector space   over the field   their tensor product is the multilinear form

 [12]

This is a special case of the product of tensors if they are seen as multilinear maps (see also tensors as multilinear maps). Thus the components of the tensor product of multilinear forms can be computed by the Kronecker product.

Tensor product of sheaves of modulesEdit

Tensor product of line bundlesEdit

Tensor product of fieldsEdit

Tensor product of graphsEdit

It should be mentioned that, though called "tensor product", this is not a tensor product of graphs in the above sense; actually it is the category-theoretic product in the category of graphs and graph homomorphisms. However it is actually the Kronecker tensor product of the adjacency matrices of the graphs. Compare also the section Tensor product of linear maps above.

Monoidal categoriesEdit

The most general setting for the tensor product is the monoidal category. It captures the algebraic essence of tensoring, without making any specific reference to what is being tensored. Thus, all tensor products can be expressed as an application of the monoidal category to some particular setting, acting on some particular objects.

Quotient algebrasEdit

A number of important subspaces of the tensor algebra can be constructed as quotients: these include the exterior algebra, the symmetric algebra, the Clifford algebra, the Weyl algebra, and the universal enveloping algebra in general.

The exterior algebra is constructed from the exterior product. Given a vector space V, the exterior product   is defined as

 

Note that when the underlying field of V does not have characteristic 2, then this definition is equivalent to

 

The image of   in the exterior product is usually denoted   and satisfies, by construction,  . Similar constructions are possible for   (n factors), giving rise to  , the nth exterior power of V. The latter notion is the basis of differential n-forms.

The symmetric algebra is constructed in a similar manner, from the symmetric product

 

More generally

 

That is, in the symmetric algebra two adjacent vectors (and therefore all of them) can be interchanged. The resulting objects are called symmetric tensors.

Additional algebras result from quotienting by other polynomials; the general case is given by the universal enveloping algebras.

Tensor product in programmingEdit

Array programming languagesEdit

Array programming languages may have this pattern built in. For example, in APL the tensor product is expressed as ○.× (for example A ○.× B or A ○.× B ○.× C). In J the tensor product is the dyadic form of */ (for example a */ b or a */ b */ c).

Note that J's treatment also allows the representation of some tensor fields, as a and b may be functions instead of constants. This product of two functions is a derived function, and if a and b are differentiable, then a */ b is differentiable.

However, these kinds of notation are not universally present in array languages. Other array languages may require explicit treatment of indices (for example, MATLAB), and/or may not support higher-order functions such as the Jacobian derivative (for example, Fortran/APL).

See alsoEdit

NotesEdit

  1. ^ See Tensor or Tensor (intrinsic definition).
  2. ^ This similar to how the engineering use of " " specifically returns the remainder, one of the many elements of the   equivalence class.
  3. ^ Hazewinkel, Michiel; Gubareni, Nadezhda Mikhaĭlovna; Gubareni, Nadiya; Kirichenko, Vladimir V. (2004). Algebras, rings and modules. Springer. p. 100. ISBN 978-1-4020-2690-4.
  4. ^ "Archived copy". Archived from the original on 2017-09-02. Retrieved 2017-09-02.CS1 maint: archived copy as title (link)[user-generated source]
  5. ^ Bourbaki (1989), p. 244 defines the usage "tensor product of x and y", elements of the respective modules.
  6. ^ Analogous formulas also hold for contravariant tensors, as well as tensors of mixed variance. Although in many cases such as when there is an inner product defined, the distinction is irrelevant.
  7. ^ "The Coevaluation on Vector Spaces". The Unapologetic Mathematician. 2008-11-13. Archived from the original on 2017-02-02. Retrieved 2017-01-26.
  8. ^ See Compact closed category.
  9. ^ Hungerford, Thomas W. (1974). Algebra. Springer. ISBN 0-387-90518-9.
  10. ^ Chen, Jungkai Alfred (Spring 2004), "Tensor product" (PDF), Advanced Algebra II (lecture notes), National Taiwan University, archived (PDF) from the original on 2016-03-04
  11. ^ Abo, H.; Seigal, A.; Sturmfels B. arXiv:1505.05729 [math.AG]
  12. ^ Tu, L. W. (2010). An Introduction to Manifolds. Universitext. Springer. p. 25. ISBN 978-1-4419-7399-3.

ReferencesEdit