We define the frame S (the lab frame) by the condition of the problem. In this frame the mirror is moving with velocity v (along say x - axis) towards left and light of frequency ω0 is approaching it from the left. We introduce the frame S ' whose axes are parallel to those of S but which is moving with velocity v along x axis towards left (so that the mirror is at re st in S'). In S' the frequency of the incident light is

In S.' the reflected light still has frequency ω0 but it is now moving towards left. When we transform back to S this reflected light has the frequency
