Thomson cross section

σe=6.6524587051×1029 m2\sigma_{\mathrm{e}} = 6.6524587051 \times 10^{-29}\ \text{m}^{2}
Value6.6524587051e-29 m²
StatusMeasured: ± 6.20e-39 m² (9.3e-11 relative)
SourceCODATA 2022
CategoriesUniversal & Atomicphysicsastrophysics
σ_e in every area unit
square millimeter6.6524587e-23 mm²
square centimeter6.6524587e-25 cm²
square meter6.6524587e-29
hectare6.6524587e-33 ha
square kilometer6.6524587e-35 km²
square inch1.0311332e-25 in²
square foot7.1606470e-28 ft²
square yard7.9562744e-29 yd²
acre1.6438583e-32 ac
square mile2.5685287e-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.