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Suppose a vector space V is defined on a field F. Does this at all imply that V is also defined on all fields, or does it only dictate that V is defined on F (and could also work with other fields if proven)?

I realize it's sort of silly to assume anything in math, but my confusion comes from examples of vector spaces that I've seen, such as n-tuples of a field with coordinate-wise addition and scalar multiplication holding for any arbitrary field.

Thanks a lot.

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    Ah, that makes sense. Thanks.2011-03-31

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A priori, if we have an abelian group $V$ (the abelian group structure provides the addition of a vector space), and we give it the structure of a vector space over a field $F$, then we only know how to make $V$ a vector space over $F$, and over any subfield of $F$. This is because when we give $V$ the structure of a vector space over $F$, the information we have specified is how to multiply elements of $V$ by elements of $F$. If $L\subset F$ is a subfield of $F$, then we already know how to define multiplication of elements of $V$ by elements of $L$: elements of $L$ are also elements of $F$, and we just use our definition for them!

For example, the collection of ordered pairs of complex numbers, $V=\mathbb{C}^2$, is an abelian group under the usual addition $(\alpha_1,\alpha_2)+(\beta_1,\beta_2)=(\alpha_1+\beta_1,\alpha_2+\beta_2) \text{ for all }(\alpha_1,\alpha_2),(\beta_1,\beta_2)\in V .$ It can be given the structure of a vector space over $\mathbb{C}$ by defining $\lambda(\alpha_1,\alpha_2)=(\lambda\alpha_1,\lambda\alpha_2)\text{ for all }\lambda\in\mathbb{C},\,\,(\alpha_1,\alpha_2)\in V.$ But, now that we've done that, it is also a vector space over $\mathbb{R}$, which is a subfield of $\mathbb{C}$ - we know how to multiply elements of $V$ by real numbers because we already have specified how to multiply by complex numbers.

However, the abelian group $V$ cannot be given the structure of a vector space over $\mathbb{Z}/p\mathbb{Z}$ where $p$ is a prime number, which is a field that is not a subfield of $\mathbb{C}$. This is because we would have to have $p\cdot (\alpha_1,\alpha_2)=(p\alpha_1,p\alpha_2)=0$ for any $(\alpha_1,\alpha_2)\in V$, which is false.

Finally, I would point out that even if $L$ is not a subfield of $F$, that doesn't prevent $V$ from also being able to be given the structure of a vector space over $L$. In our example of $V=\mathbb{C}^2$, suppose we had originally specified that $V$ was to be considered as a vector space over $\mathbb{R}$. That is, suppose we had said, "Here is our abelian group $V=\mathbb{C}^2$, and we make it into a vector space over $\mathbb{R}$ by defining c(\alpha_1,\alpha_2)=(c\alpha_1,c\alpha_2)\text{ for all }c\in\mathbb{R},\,\,(\alpha_1,\alpha_2)\in V." This wouldn't change the fact that it can also be given the structure of a vector space over $\mathbb{C}$, in a way that agrees with the original structure over $\mathbb{R}$, even though $\mathbb{C}$ is a larger field than $\mathbb{R}$.

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    @Qiaochu: Fair point; I was glossing over this point given the level of the OP, but I'll edit.2011-03-30
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Many of the constructions of vector spaces do not depends on the specific field. Category theory can help to explain why this is since the constructions are really category theory constructions which don't use any property of the field. However, some constructions do use properties of the field, and there isn't any obvious analogue over other fields. For example, smooth functions $\mathbb{R} \to \mathbb{R}$ form a real vector space, and there isn't a natural analogue over the field with $2$ elements.

If you have fields $K \subset L$ (such as $\mathbb{R} \subset \mathbb{C}$) then for any $K$-vector space $V$, there is a natural way to construct an $L$-vector space, $V \otimes_K L$. This is generated by elements of the form $v \otimes \ell$ where $v\in V$ and $\ell \in L$, with rules including $v_1 \otimes \ell + v_2 \otimes \ell = (v_1+v_2)\otimes \ell$, $v \otimes \ell_1 + v\otimes \ell_2 = v\otimes (\ell_1+\ell_2)$, and $k v \otimes \ell = v \otimes k \ell$. Tensor products over $K$ of $K$-vector spaces are always $K$-vector spaces, but these also have the structure of an $L$-vector space because you can multiply the second coordinate by a scalar from $L$. You can identify $V$ with the set of elements of the form $v \otimes 1$.

Also, if you have fields $K \subset L$, then any $L$-vector space is also a $K$-vector space.

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    Finite-dimensional vector spaces which are defined by a basis can be given coefficients in any field. They are an example of a [free object](http://en.wikipedia.org/wiki/Free_object).2011-03-30