Left Invariant vector field on SO(3) I have a Lie group, namely on SO(3), i.e. $SO(3,\mathbb{\mathbb{R}})=\left\{ A\in GL\left(3,\mathbb{R}\right)\mid A^{T}A=\mathbb{1},\,\det\left(A\right)=1\right\}$. 
I have a Left action $L_g$ and I know that by definition a left invariant vector field is a vector field such that
$$(L_g)_{\ast}(X_e)=X_g$$
I worked out few thing with the tangent space at the identity and I arrived at formulating the idea that this should be a left invariant vector field on $SO(3)$:
$$L_{\mathbf{1}}=y\frac{\partial}{\partial z}-z\frac{\partial}{\partial x}$$
But now how to I effectively demonstrate that is left invariant. Can anybody show me the computation that once in a lifetime must be seen? Or at least give a refernce that actually shows the computation technique?
 A: This kind of formula only works when you have the action of the lie group $G = SO(3)$ on some manifold $M$, in this case, the euclidean space $\mathbb{R}^3$. Let then $G$ act on $M$ by $(g,x) \mapsto gx$. 
A left-invariant vector field $V$ in $G$ induces a vector field on $M$ such that the flow in $M$ is: $${\gamma(t,x) = \exp(tV)x,}$$ where $\exp: \mathfrak{g} \rightarrow G$ is the exponential map. Define the induced vector field $\tilde{V}$ on $M$ by: $${\tilde{V} = \frac{d}{dt}\exp(tV)x|_{t=0}.}$$Then we have defined a map $\mathfrak{g} \rightarrow \mathfrak{X}(M)$ by $V \mapsto \tilde{V}$. 
In your case, take an element of $\mathfrak{so}(3)$ (the lie algebra of $SO(3)$, e.g.: the tangent space at the identity), namely: 
$$X = \begin{bmatrix}
0 & 0 & 0\\ 
0 & 0 & -1\\
0 & 1 & 0
\end{bmatrix}$$
(You can see that this is an element of $\mathfrak{so}(3)$ because it is an antissymetric matrix). 
Then your induced vector field is $\tilde{X} = -z\frac{\partial}{\partial y} + y \frac{\partial}{\partial x}$.
