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tensor product basis (Theorem)

The following theorem describes a basis of the tensor product of two vector spaces, in terms of given bases of the component spaces. In passing, it also gives a construction of this tensor product. The exact same method can be used also for free modules over a commutative ring with unit.

Theorem. Let $U$ and $V$ be vector spaces over a field $\K$ with bases $$ \{\vek{e}_i\}_{i \in I} \quad\text{and}\quad \{\vek{f}_j\}_{j \in J} $$ respectively. Then \begin{equation} \label{Eq:ProdBas} \{ \vek{e}_i \otimes \vek{f}_j\}_{(i,j) \in I \times J} \end{equation}is a basis for the tensor product space $U \otimes V$ .

Proof. Let $$ W = \setOfBig{ \psi\colon I \times J \Fpil \K }{ f^{-1}\bigl( \K \setminus \{0\} \bigr) \text{ is finite} }\text{;} $$ this set is obviously a $\K$ -vector-space under pointwise addition and multiplication by scalar (see also this article). Let $ p\colon U \times V \longrightarrow W$ be the bilinear map which satisfies
$\displaystyle p(\mathbf{e}_i,\mathbf{f}_j)(k,l) = \begin{cases}1& \text{if \(i=k\) and \(j=l\),}\\ 0& \text{otherwise} \end{cases}$ (1)

for all $ i,k \in I$ and $ j,l \in J$, i.e., $ p(\mathbf{e}_i,\mathbf{f}_j) \in W$ is the characteristic function of $\bigl\{(i,j)\bigr\}$ . The reasons (1) uniquely defines $p$ on the whole of $U \times V$ are that $\{\vek{e}_i\}_{i \in I}$ is a basis of $U$ , $\{\vek{f}_i\}_{j \in J}$ is a basis of $V$ , and $p$ is bilinear.

Observe that $$ \bigl\{ p(\vek{e}_i,\vek{f}_j) \bigr\}_{(i,j) \in I \times J} $$ is a basis of $W$ . Since one may always define a linear map by giving its values on the basis elements, this implies that there for every $\K$ -vector-space $X$ and every map $ \gamma\colon U \times V \longrightarrow X$ exists a unique linear map $ \widehat{\gamma}\colon W \longrightarrow X$ such that $$ \widehat{\gamma}\bigl( p(\vek{e}_i,\vek{f}_j) \bigr) = \gamma(\vek{e}_i,\vek{f}_j) \quad\text{for all \(i \in I\) and \(j \in J\).} $$ For $\gamma$ that are bilinear it holds for arbitrary $ \mathbf{u} = \sum_{i \in I'} u_i\mathbf{e}_i \in U$ and $ \mathbf{v} = \sum_{j \in J'} v_j\mathbf{f}_j \in V$ that $ \gamma(\mathbf{u},\mathbf{v}) = (\widehat{\gamma} \circ\nobreak p)(\mathbf{u},\mathbf{v})$, since

\begin{multline*} \gamma(\mathbf{u},\mathbf{v}) = \gamma\biggl( \sum_{i \in I'} ... ... \widehat{\gamma}\bigl( p(\mathbf{u},\mathbf{v}) \bigr) \text{.} \end{multline*}

As this is the defining property of the tensor product $U \otimes V$ however, it follows that $W$ is (an incarnation of) this tensor product, with $ \mathbf{u} \otimes \mathbf{v} := p(\mathbf{u},\mathbf{v})$. Hence the claim in the theorem is equivalent to the observation about the basis of $W$ . $ \qedsymbol$




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See Also: tensor product, free vector space over a set

Other names:  basis construction of tensor product
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Cross-references: equivalent, defining property, map, implies, linear map, bilinear, characteristic function, bilinear map, scalar, multiplication, pointwise addition, field, unit, commutative ring, free modules, vector spaces, basis, theorem
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This is version 8 of tensor product basis, born on 2005-07-25, modified 2007-09-01.
Object id is 7254, canonical name is TensorProductBasis.
Accessed 4160 times total.

Classification:
AMS MSC15A69 (Linear and multilinear algebra; matrix theory :: Multilinear algebra, tensor products)

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