Processes where gamma rays interact with matter for detection, medical use, or nuclear studies.Gamma-ray interactions with matter describe the physical processes by which high-energy photons transfer energy to atoms and particles. The three dominant mechanisms are the photoelectric effect, Compton scattering, and pair production, each dominating in different energy ranges and for different absorber materials. These interactions are fundamental to detecting gamma rays, shielding against radiation, and using gamma rays in medical treatments and nuclear research.
The photoelectric effect was explained by Albert Einstein in 1905, Compton scattering by Arthur Compton in 1923, and pair production was predicted by Paul Dirac in 1928 and confirmed experimentally in 1933 by Patrick Blackett and Giuseppe Occhialini.
In the photoelectric effect, a gamma photon is absorbed by an atom, ejecting an inner-shell electron with energy equal to the photon energy minus the binding energy. Compton scattering involves the photon bouncing off a free or loosely bound electron, transferring part of its energy and changing direction. At energies above 1.022 MeV, pair production occurs near a nucleus: the photon converts into an electron-positron pair, with the excess energy becoming kinetic energy. The cross-sections for these processes depend on photon energy and the atomic number of the material, which is why high-Z materials like lead are effective shields.
Gamma-ray interactions are exploited in radiation therapy for cancer (using pair production and Compton scattering to deposit energy in tumors), in gamma spectroscopy for nuclear analysis, and in designing radiation shielding for reactors and spacecraft.
In Compton scattering, the wavelength shift of the scattered photon depends only on the scattering angle, not on the photon's initial energy—a fact used in Compton cameras for medical imaging.
| \sigma | variable | Cross section — cross section square metre |
| g_1 | variable | Coupling constant of particle 1 — coupling constant joule metre |
| g_2 | variable | Coupling constant of particle 2 — coupling constant joule metre |
| \mu | variable | Reduced mass of the two-particle system — mass kilogram |
| m | variable | Mass scale (typically the mass of the particles) — mass kilogram |






