In the Einstein's parallel mirrors experiment, when the light pulse strikes the opposite mirror, there should appear an interferential picture.
My Gilette mirror experiment shows - the picture appears between the falling on the mirror beam and the reflected one. This means we see the light pulse's side along some perpendicular line, with light pulse being some length (e.g.). The more close to the surface of the mirror the falling beam is, the more circles (fringes) there in the picture should be, which means ...
my interferential picture is an embodiment of famous equation (1 - v2/c2)-1/2.
This SQR equation itself is sin of the angle, with which the falling beam falls upon the mirror's surface and means:
assuming Newton - c'/c (relative speed/absolute speed)
assuming Einstein - t'/t (relative time/absolute time).
See Einstein experiment with innovations: light pulse is longer (moves by its side relatively), and with interferential picture:
http://www.relativity.hotmail.ru/Parallel_Interferential.htm
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