Align the spatial axes and make the origins coincide at . For an inertial frame moving at velocity along , the Lorentz transformation is
The inverse Lorentz transformation follows by interchanging primed and unprimed coordinates and replacing by .
Let the object be at rest in , with proper length . Measuring its length in requires two endpoint events simultaneous in , so . The Lorentz transformation then gives
This is length contraction. The simultaneous endpoint events in are not simultaneous in ; that relativity of simultaneity is essential to the measurement.
For the two rockets, take the first rocket's Earth-frame velocity as and the second's as . The velocity-addition formula gives the second rocket's velocity in the first rocket's rest frame:
Its Lorentz factor is , and therefore its measured length is
Here “appear” is interpreted as a length measured using simultaneous endpoint positions in the observer's inertial frame. A photograph, involving unequal light travel times, is a different measurement.
Write the incident and scattered photon energies as and . Conservation of relativistic energy gives the recoiling electron energy . By momentum conservation, its momentum is the difference of the two photon momenta; hence
Insert these into the relativistic energy-momentum relation for the electron:
Expanding and cancelling terms gives
Since , the Compton scattering formula follows:
The scale is the electron Compton wavelength. At , : there is no energy or momentum transfer in this ideal forward limit, so the electron remains at rest. At , the wavelength shift is maximal:
The electron gains its largest kinetic energy, , and recoils forward while the photon reverses direction.

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