Compton edge

Gamma-spectrum of a radioactive Am-Be-source. The photopeak after the Compton edge corresponds to detection of the incident gamma rays. The significantly lower count in the region between the Compton edge and the photopeak reflects the fact that no gamma rays of this energy can be absorbed by the detector.

In a Compton scattering process, an incident photon collides with an electron in a material. The amount of energy exchanged varies with angle, and is given by the formula:

${\displaystyle {\frac {1}{E^{\prime }}}-{\frac {1}{E}}={\frac {1}{m_{\text{e}}c^{2}}}\left(1-\cos \theta \right)}$

or

${\displaystyle E^{\prime }={\frac {E}{1+{\frac {E}{m_{\text{e}}c^{2}}}(1-\cos \theta )}}}$ [1]

• E is the energy of the incident photon.
• E' is the energy of the outgoing photon, which escapes the material.
• ${\displaystyle m_{\text{e}}}$ is the mass of the electron.
• c is the speed of light.
• ${\displaystyle \theta }$ is the angle of deflection for the photon.

The amount of energy transferred to the material varies with the angle of deflection. As ${\displaystyle \theta }$ approaches zero, none of the energy is transferred. The maximum amount of energy is transferred when ${\displaystyle \theta }$ approaches 180 degrees.

${\displaystyle E_{T}=E-E^{\prime }}$

${\displaystyle E_{\text{Compton}}=E_{T}({\text{max}})=E\left(1-{\frac {1}{1+{\frac {2E}{m_{\text{e}}c^{2}}}}}\right)}$

It is impossible for the photon to transfer any more energy via this process, hence there is a sharp cutoff at this energy giving rise to the name Compton edge.

The region between zero energy transfer and the Compton edge is known as the Compton continuum.

• Gamma spectroscopy
• Compton suppression