I'm not sure if this question would be more appropriate in Physics.SE, if so let me know.
I need help in understanding this quote from "Arnold - Mathematical Methods in Classical Mechanics" (This is my translation from italian):
The affine $n$-dimensional space $A^n$ differs from $\mathbb R^n$ for the fact that there's no fixed origin in it. The group $\mathbb R ^n$ acts in $A^n$ like the group of parallel transport: $$\mathbf a \rightarrow a+\mathbf b \quad (a\in A^n, \mathbf b \in \mathbb R^n, a+\mathbf b\in \mathbb R^n)$$(in this way, the sum beetween two points in $A^n$ is undefined, but the difference is defined as a vector of $\mathbb R^n$.)
I have different questions:
- Why is $\mathbb R ^n$ referred as a "group"? Is it referred to $\mathbb R ^n$ being a group under the operation of sum?
- What does that mapping mean? Also, am I right in suspecting that the bold character in first $\mathbf a$ is a typo?
- In other places, I've seen the sum beetween a point $p\in A^n$ and a vector of $\mathbf v \in \mathbb R ^n$ defined as the unique point $q\in A_n$ such that $f(p,q)=\mathbb v$, where $f$ is the function that gives to $A^n$ the affine structure. If this is the case (and I'm not sure about it) how does this define the difference beetween two points?
This question seems perfectly on topic here.
The vector space $\mathbb{R}^n$ is a group under addition - you should check the axioms yourself if you haven't seen this before.
I agree that there is a typo in the mapping. This is a map $f\colon A^n\times\mathbb{R}^n\to A^n$ given by $f(a,\mathbf{b})=a+\mathbf{b}$. If you're familiar with the terminology of group actions, this is an action of $\mathbb{R}^n$ on $A^n$ (and because $\mathbb{R}^n$ is abelian, we don't have to worry about whether it is a left or right action).
Now, given two points $a,b\in A^n$, there is a unique $\mathbf{v}$ such that $f(a,\mathbf{v})=b$, and we define $b-a=\mathbf{v}$ (note that while $a,b\in A^n$, their difference is in $\mathbb{R}^n$).
Some Extra Detail: The reason this works is that $\mathbb{R}^n$ acts freely and transitively on $A^n$, meaning that if $f(a,\mathbf{v})=a$ for all $a\in A^n$ then $\mathbf{v}=0$, and that for all $a,b\in A^n$ there exists $\mathbf{v}\in\mathbb{R}^n$ with $f(a,\mathbf{v})=b$. Any set with a group acting freely and transitively on it is called a torsor for the group, and behaves like a "group without an identity" (compare to "vector space without an origin"). You can always define subtraction (or division if you're using multiplicative notation) in a torsor in this way; the difference $y-x$ of two elements of the torsor is the unique element of the group that acts by taking $x$ to $y$.