Proof:

We first show that the action is well-defined. That is to say if $ \gamma_1$ and $ \gamma_2$ are homotopic loops based at $ x_0$ then for $ {\tilde x}\in p^{-1}(x_0)$

$\displaystyle {\tilde \gamma}_1(1) = {\tilde \gamma}_2(1),
$

where $ {\tilde \gamma}_1$ and $ {\tilde \gamma}_2$ are lifts of $ \gamma_1$ and $ \gamma_2$ starting at $ {\tilde x}$. Well, if $ F$ is the homotopy between $ \gamma_1$ and $ \gamma_2$ then $ F$ has a unique lift $ {\tilde F}$ satisfying $ {\tilde F}(0, 0) = {\tilde x}$. In other words, $ {\tilde F}: [0, 1]\times [0, 1]\longrightarrow {\tilde X}$ is the unique continuous map such that

$\displaystyle p\circ {\tilde F} = F,\quad {\tilde F}(0, 0) = {\tilde x}
$

In particular the image set $ \{{\tilde F}(s, 1)\}$ as $ s$ runs through $ [0, 1]$, must be a connected subset of $ {\tilde X}$. But since $ F$ is a homotopy of loops based at $ x_0$,

$\displaystyle F(s, 1) = p\circ {\tilde F}(s, 1) = x_0,$    for all $\displaystyle s \in [0, 1].$

Hence $ \{{\tilde F}(s, 1)/ s\in [0, 1]\} \subset p^{-1}(x_0)$ which means $ \{{\tilde F}(s, 1)/ s\in [0, 1]\}$ is a singleton since $ p^{-1}(x_0)$ is discrete. In particular,

$\displaystyle {\tilde F}(0, 1) = {\tilde F}(1, 1),$    that is, $\displaystyle \quad {\tilde \gamma}_1(1) = {\tilde \gamma}_2(1).
$

Next, we show that (15.1) defines a right group action. First let us note that if $ {\tilde x}_1, {\tilde x}_2$ and $ {\tilde x}_3$ are three points in $ p^{-1}(x_0)$ and $ {\tilde \gamma}_1$ and $ {\tilde \gamma}_2$ is a pair of paths joining $ {\tilde x}_1$ to $ {\tilde x}_2$ and $ {\tilde x}_2$ to $ {\tilde x}_3$ respectively then

$\displaystyle p\circ({\tilde \gamma}_1*{\tilde \gamma}_2) = (p\circ{\tilde \gamma}_1) * (p\circ{\tilde \gamma}_2).
$

Now let $ \gamma_1$ and $ \gamma_2$ be two loops in $ X$ based at $ x_0$. Assume that $ {\tilde \gamma}_1$ is the unique lift of $ \gamma_1$ starting at $ {\tilde x}_1$ and $ {\tilde \gamma}_2$ is the unique lift of $ \gamma_2$ starting at the point $ {\tilde x}_2 = {\tilde \gamma}_1(1)$ then the juxtaposition $ {\tilde \gamma}_1*{\tilde \gamma}_2$ is defined and is the unique lift of $ \gamma_1 * \gamma_2$ starting at $ {\tilde x}_1$. Thus,
$\displaystyle {\tilde x}_1\cdot([\gamma_1][\gamma_2]) = {\tilde x}_1\cdot[\gamma_1*\gamma_2] = {\tilde \gamma_1}*{\tilde \gamma}_2(1) = {\tilde \gamma}_2(1)$      

On the other hand,

$\displaystyle {\tilde \gamma}_2(1) = {\tilde x}_2\cdot[\gamma_2] = ({\tilde x}_1\cdot [\gamma_1])\cdot [\gamma_2].
$

Note that if we had tried to operate from the left we would instead get an anti-action. This is one of the instances where it is important to have the book-keeping done correctly from the very outset.

Finally the constant loop $ \varepsilon_{x_0}$ at $ x_0$ lifts as the constant loop starting at $ {\tilde x}_1\in p^{-1}(x_0)$ and so (17.1) implies

$\displaystyle {\tilde x}_1\cdot [{\varepsilon}_{x_0}] = {\tilde x}_1,\quad {\tilde x}_1\in p^{-1}(x_0).
$

We now examine the issues related to this group action namely, its transitivity and the stabilizer subgroups of various points of $ p^{-1}(x_0)$.

nisha 2012-03-20