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I find that the best solution to relativity conundrums is to apply the
Lorentz transformations.
Let the light enter the train at the origin in both reference frames. The
train moves in the +x direction according to the track frame. The light
moves across the track in the +y direction in the track frame. The width
of the train is w, same in both frames.
In track frame, time of light leaving train is simply w/c. Location of
that event is x=0, y=w, t=w/c.
Now plug those numbers into the Lorentz transformations to find the
spacetime locations for the leaving-train event in the train frame.
x' = gamma * (0 - v*t) = - gamma * v * w / c
y' = w
t' = gamma *(t - (v/c^2)x) = gamma * w/c