Visualization of Lie groups

Proposition
Given a group action G×MM free and transitive, fixed mM we have a bijection

GM

with ggm

See principal homogeneous spaces in homogeneous space .
This result can be proven easily and let us use the manifold M to visualize G.

If the action is not free (but still transitive), we cannot visualize G (for example, SO(3) acting over S2). Anyway, observe first that the stabilizer of every xM are all conjugate of each other. And second, if we fix xM, we can establish a surjection πx:GM, πx(g)=gx, that gives rise to a bijection

π¯x:G/GxX

From here we have a natural bijection

GmM{m}×πx1(m)

that could be translated to a bijection

GM~=mM{m}×Gm

if we had a \textit{preferred choice} of a tmG such that tmx=m for every mM (need to be proven but I think is easy). Take g(gx,gtgx1)...
In this circumstances, we can even define an action of G at M~:

(g,(m,h))(gm,ghg1)

But it is not necessarily transitive or free.

But on the other hand, since the action of G on itself is free and transitive, we can copy this action to M~ with the previous bijection and obtain a new action on M~

(g,(m,h))(gm,ghtmtgm1)

For example, we can see SO(3) as the sphere bundle of S2. Remember

SM:={(x,v):xM,vTxM,|v|=1}==xM{x}×S1

This is this way because if we fix a point P in S2 and define πP:SO(3)S2 taking the action on P, we have the bijection of SO(3) with {x}×πP1(x) and, even more, we have preferred transformations from one point to another: the great circle paths \textbf{with angle lesser or equal to π}. So (following result above) we have

SO(3)xS2{x}×SO(2)

given explicitly by

g(gP,gtgP1)

where tQ is the great circle path from P to Q.
This bijection is, indeed, a diffeomorphism, as can be proven with the map

Φ:S(S2)SO(3)Φ(x,v):=[x,v,x×v]

that sends the pair of vectors in R3 (x,v) to the orthogonal matrix [x,v,x×v].

But let's return to our original map and take P=(1,0,0) and think of several examples to \textit{see} the elements of SO(3).

To sum up, we would have something like this: fixed PS2, rotations around great circles passing through P and angle θ are encoded in the arrival point of P, Q. If the rotation is not along a great circle, is encoded in the same final point Q but with an \textit{internal rotation} of angle γ (i.e., an element of the SO(2) of Q) related to the angular displacement α of the axis of the rotation respect to the ideal great circle rotation taking P to Q with angle lesser than π. By mean of examples I guess that γ=2α:
rotations3.jpg|400
Possible rotations other than the great circle of axis ePQ taking P to Q arise when we choose a different axis e along the \textit{perpendicular bisector} of PQ. The extremal case is when e=ePQ (α=π), and then they begin to be repeated (although in a complementary way).
Keep an eye: this is not diffeomporhic to the 3-sphere S3. S3 is diffeomorphic to the covering group SO(3)~=SU(2), the double cover of SO(3). See unitary matrix#Unitary matrix#What is SU 2 topologically.