How does a laser beam change angle from frame to frame in special relativity? I am at Point A, and I have a laser pointer. I point it at a mirror, one mile west of me, at point B. The beam travels to the mirror and comes back to make a nice round dot on my shirt at point C. In my frame, Points A and C are the same.
Bob zooms over me in his spaceship, going half the speed of light due north. Since he is going half the speed of light, he travels one mile in the time it takes my laser to go two miles. In his frame, he sees my laser fire at point A, hit the mirror at B, and reflect to point C, which is a long ways south of Point A. 
As we all know, the Lorentz transformation arranges everything so that both of us see the light beam traveling at speed $c$. But the Lorentz transformation does not change the fact that my laser is pointed due west, in my frame and in Bob's frame. Yet Bob sees the beam travel at an angle, and reflect at the opposite angle, to arrive well south of where it originated.
In my frame, the laser is stationary, and the beam it emits travels parallel to its axis. In Bob's frame, the laser is moving south at half the speed of light. How does that motion cause the beam to be produced at an angle to the laser's axis?
 A: Let's have a closer look at your laser projector in your rest frame. In particular let's concentrate on a single photon inside the projector:

Actually I've just realised I've drawn my diagram with the laser moving East not West - oh well. Anyhow in this frame the laser beam moves due East in a straight line. So far so good.
Now let's look at the situation in Bob's frame:

In Bob's frame the laser projector is moving with time at 0.5$c$. The projector still points due east, but the photon making its way along the projector towards the exit window is now not travelling due east but instead is travelling at a diagonal.
So the point is that the laser projector does not need to be rotated for the beam to emerge at an angle.
A: Angle of emission $\theta_s$ and angle of reception $\theta_o$ are tied by relativistic aberration formula.
$$ \cos {\theta_0} = \frac {\cos {\theta_s} - \frac v c} {1- \frac v c \cos \theta_s} $$
This simple animation demonstrates path of laser beam in different frames:
https://www.youtube.com/watch?v=FQKp3FU8vR8
By the way. Angles are different, and observations are different. What about provisions of Special Relativity?
