Thomson cross section
| Value | 6.6524587051e-29 m² |
| Status | Measured: ± 6.20e-39 m² (9.3e-11 relative) |
| Source | CODATA 2022 |
| Categories | Universal & Atomicphysicsastrophysics |
| square millimeter | 6.6524587e-23 mm² |
| square centimeter | 6.6524587e-25 cm² |
| square meter | 6.6524587e-29 m² |
| hectare | 6.6524587e-33 ha |
| square kilometer | 6.6524587e-35 km² |
| square inch | 1.0311332e-25 in² |
| square foot | 7.1606470e-28 ft² |
| square yard | 7.9562744e-29 yd² |
| acre | 1.6438583e-32 ac |
| square mile | 2.5685287e-35 mi² |
Learning zone
σ_T = (8π/3)r_e² is the effective target area a free electron presents to a photon whose energy is far below 511 keV, derived classically by J. J. Thomson from an electron shaken by an oscillating field and re-radiating. It is independent of frequency, which is exactly why it fails for hard photons: above roughly 100 keV, Compton recoil takes over and the Klein-Nishina formula drives the cross section down.
This constant runs astrophysics. It fixes the Eddington luminosity, the point at which radiation pressure on electrons balances gravity and a star blows off its own envelope; it sets the optical depth of the ionised intergalactic medium, whose Thomson scattering of the cosmic microwave background is measured by Planck as τ ≈ 0.054 and used to date reionisation; and it governs how photons random-walked out of the primordial plasma before recombination. In the barn units nuclear physicists use, σ_T = 0.665 b.