Section 2.1 Definition of a vector space
Let \(V\) be an abelian group. We write the binary operation on \(V\) additively. Thus \((V,+)\) have the following properties:
For \(v,w\in V\text{,}\) \(v+w=w+v\text{.}\)
For \(v,w,z\in V\text{,}\) \(v+(w+z)=(v+w)+z\text{.}\)
There exists a unique element \(0\in V\) such that for any \(v\in V\text{,}\) \(0+v=v+0=v\text{.}\)
For every \(v\in V\) there exists a unique element (which is denoted by \(-v\)) such that \(v+(-v)=(-v)+v=0\text{.}\)
Now we give the definition of a vector space over a field. Let \(1\) be the unity in \(F\text{.}\) Then,
Definition 2.1.1. (Vector space over a field).
Let \(F\) be a field and let \(V\) be an abelian group. We call \(V\) a vector space over \(F\) or an \(F\)-vector space if there is a map, called scalar multiplication
For \(\alpha,\beta\in F\) and \(v\in V\text{,}\) we have
For \(\alpha\in F\) and \(v,w\in V\) we have
For \(\alpha,\beta\in F\) and \(v\in V\text{,}\) we have
Remark 2.1.2.
Often we omit "\(\cdot\)" for scalar multiplication and simply write \(\alpha v\text{.}\)Remark 2.1.3.
Please try not to confuse the terminology of a vector that you have studied in 12th, viz., a vector is something that has a 'length', 'base', and it is denoted by an arrow, etc.. The definition above is what we will use throughout!Example 2.1.4.
If we fix \((1,1)\in\R^2\) then, for given \(\alpha\in\R\) we get
In this way, we may say that \(\R\) sits inside \(\R^2\text{.}\)