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The spectrum of radiation at an angle consists of two peaks, one at and the other at . Compton effect can be explained by assuming that the incoming radiation is a beam of particles with |
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In arriving at the last relationship, we use the energy - momentum relation of the special theory of relativity , according to which, |
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where is the rest mass of a particle. Since photons are massless ( ), we get . Compton's observation is consistent with what we expect if photons, considered as particles, collide with electrons in an elastic collision. |