Linear algebra (Osnabrück 2024-2025)/Part II/Lecture 56

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Base change for tensor product

Let be a field, and let denote finite-dimensional vector spaces over . Let , and , be bases of , with the base change matrices

Then the base change matrix

(with ) between the bases

of the tensor product is given by the -matrix with the entries

Due to the definition of the base change matrix, we have

Therefore, using Lemma 55.9   (3), we obtain

and these coefficients constitute the base change matrix.



We consider with den bases , and the standard basis . We consider as a real vector space with the bases and . Hence, the base change matrices, as they appear in Lemma 56.1 , are

and

We use the ordering , and obtain the base change matrix

For example, in the second column, we write the coefficients needed to express as a linear combination of the .



Tensor product and dual space

Let be a field, and let denote finite-dimensional vector spaces over . Then there exists a natural isomorphism

For fixed linear forms , the mapping

is multilinear due to Exercise 16.39 ; therefore, it defines a linear form on . This yields the mapping

This assignment is also multilinear, and gives a linear mapping

Due to Corollary 55.13 and Corollary 13.12 , both spaces have the same dimension. Let , , be bases of . Then the form, according to Theorem 55.12   (3), a basis of , and the dual basis is a basis of the dual space. We claim the equality of the linear mappings

This equality follows from the fact that both mappings give, when applied to the basis elements , in case the value , and else the value . Therefore, is surjective, and then also injective.



Let be a field, and let denote -vector spaces. Then the following statements hold.

(in the sense of a canonical isomorphy).
  1. We have
  2. We have

Proof

See Exercise 56.2 .




Tensor product of linear mappings

Let be a field, and let denote vector spaces over . Let

be -linear mappings. Then there exists a well-defined linear mapping

with

The composed mapping

is multilinear according to Exercise 16.13 . Therefore, due to Theorem 55.4 , this induces a linear mapping



Let be a field, and let denote vector spaces over . For -linear mappings

the linear mapping

is called the tensor product

of the . It is denoted by .

Let be a field, and let denote vector spaces

over . Then the following statements hold.
  1. For a -linear mapping , there exists a natural -linear mapping .
  2. If is surjective, then also is surjective.
  3. If injective is, then also is injective.

(1). This is a special case of Lemma 56.5 .

(2). The surjectivity of the mapping

is clear, because the form a -generating system of , and these belong to the image of the mapping.

(3). Because of the injectivity, we may assume that

is a linear subspace. A basis , , of can be extended to a basis , , of , with Let , , be a basis of . Then, according to Theorem 55.12   (3), the family , , is a basis of . The subset , , is a basis of . therefore, under

a basis is mapped to linearly independent elements, and thus this mapping is injective.


Therefore, for linear subspaces , the tensor product is in a natural way a linear subspace of .


Let be a field, and let denote -vector spaces. Then we have

Proof

See Exercise 56.5 .



Change of base field

We have several times simplified a real problem by considering the situation over the complex numbers. If the situation can be formulated with a real matrix, then we can consider it directly as a complex matrix, and we can compute its (non-real) complex eigenvalues. Matrices describe mathematical objects, and they depend in general on the choice of bases. The tensor product allows to describe the passage to the complex situation on the level of the objects. We consider here the case that a -vector space and a field extension are given. We fix the terminology that we will use.


A subset of a field is called a subfield of , if the following properties hold.

  1. We have .
  2. For also holds.
  3. For , also holds.
  4. For , we also have .
  5. For , , we also have .

Let be a field, and let be a subfield of . Then is called an extension field of , and the inclusion is called a

field extension.

Let be a field extension. Then is is in natural way a

-vector space.

The scalar multiplication

is simply given by the multiplication in . The vector space axioms follow directly from the field axioms.



For a -vector space over a field , and a field extension , the tensor product is called the (-)

vector space given by extension of scalars.

Instead of , we also write .


Let be a field, be a -vector space, and a

field extension. Then the following statements hold.
  1. The tensor product is an -vector space.
  2. There exists a canonical -linear mapping

    For , this is an isomorphism.

  3. For a -linear mapping , the induced mapping

    is -linear.

  4. For , we have
  5. For a finite-dimensional -vector space , we have
  6. For another field extension , we have

    (an isomorphism of -vector spaces).

(1). The multiplication

is -bilinear, and, in particular, -bilinear; therefore, it yields, according to Theorem 55.4 , to a -linear mapping

This induces, due to Lemma 56.4   (2) and Proposition 56.7 , a -linear mapping

This gives a well-defined scalar multiplication

which is explicitly given by

From this description, we can deduce directly the properties of a scalar multiplication.
(2). The -homomorphism follows directly from the bilinearity of the tensor product. For , the mapping is surjective. The scalar multiplication induces a -linear mapping

The composition of the canonical mapping with this mapping is the identity on , so that the first mapping is also injective.
(3) follows from the explicit description in (1).
(4) follows from Corollary 56.8 .
(5) follows from (4).
(6). Because of part (2), we have, one one hand, a -linear mapping . This yields a -multilinear mapping

which induces a -linear mapping

On the other hand, we have a -linear mapping

On the right-hand side, we have an -vector space; therefore, the scalar multiplication may be considered as an -multilinear mapping

This induces an -linear mapping

The two mappings are inverse to each other, as this can be checked on the decomposable tensors. This shows also that the -multiplications are the same.



Let be a field, be a -vector space, and be a field extension. Let , ,

be a family of vectors in . Then the following statements hold.
  1. The family , , is a -generating system of if and only if , , is an -generating system of .
  2. The family , , is -linearly independent in if and only if , , is linearly independent (over ) in .
  3. Die family , , is a -basis of if and only if , , is an -basis of .

Proof

See Exercise 56.15 .

Let be a real vector space. The tensorization with the -algebra , that is,

is called the complexification of . If has the dimension , then has, considered as a complex vector space, also the dimension . If we consider as a real vector space, then it has the real dimension .



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