Align the spatial axes and make the origins coincide at . For an inertial frame moving at velocity along , the Lorentz transformation isThe 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 givesThis 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 isHere “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; henceInsert these into the relativistic energy-momentum relation for the electron:Expanding and cancelling terms givesSince , 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.
Articles by others on the same topic
There are currently no matching articles.