# Compton scattering vs. photoelectric effect

Say a photon hits some atom.

What determines whether there will be a photoelectric effect (photon is absorbed, electron is released) or whether there will be a Compton scattering (the photon is scattered at some angle, and the electron is released with another direction)?

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All we can ascribe to a process like you are describing ($\gamma + p \rightarrow products$) is a probability. The sum over all process will give us %100. I couldn't find a plot of anything like the process you described, but I did find this plot of Higgs decay products as a example of the probabilistic nature of quantum mechanics. On the bottom axis is the possible higgs mass (now determined to be pretty close to 125 GeV) and on the vertical axis it says given the Higgs mass, how likely it will decay to those products.

Keep in mind calculating probabilities for hands dealt in a poker game is pretty much the same thing:

All we can do is calculate the probability for a single outcome, and all the possible outcomes add up to %100.

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I suppose I should explain my downvote. This is completely irrelevant to the question. There does exist a plot that describes the cross-section for different interactions as a function of photon energy. It has nothing to do with the Higgs. – Colin McFaul Jul 8 '12 at 2:55
@ColinMcFaul - Thanks for the explanation of your downvote. I probably didn't do a great job explaining it but my purpose of the higgs plot was to give an example of the probabilistic outcomes in quantum mechanics, and particle physics in particular. I couldn't find a plot of the form that you posted so I posted the closest type of plot I could find. – DJBunk Jul 8 '12 at 14:36

For a given system that the electron is in, the primary determinant is the energy of the photon. As @DJBunk points out, this is a quantum mechanical process, so the "choice" is fundamentally random. A given interaction will occur with a probability proportional to its cross section. Figure 1 of this lecture shows how the cross section for each possible process varies with photon energy. This plot is for the interaction of photons with electrons in copper. At low energies, the photoelectric effect is the dominant effect. From about 200 keV to about 10 MeV, Compton scattering is the dominant effect. Above 10 MeV, the dominant effect is pair production. At a given photon energy, the relative probability of two processes would be the ratio of their cross sections.

The dependence of each cross section on photon energy should be similar in form for any system; the exact numbers will vary from system to system. Table 2 of that lecture gives the dependence on the atomic number, for example.

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