Nuclear cross sections are used in determining the nuclear reaction rate, and are governed by the reaction rate equation for a particular set of particles (usually viewed as a "beam and target" thought experiment where one particle or nucleus is the "target", which is typically at rest, and the other is treated as a "beam", which is a projectile with a given energy).
For particle interactions incident upon a thin sheet of material (ideally made of a single isotope), the nuclear reaction rate equation is written as:
where:
Types of reactions frequently encountered are s: scattering, γ {\displaystyle \gamma } : radiative capture, a: absorption (radiative capture belongs to this type), f: fission, the corresponding notation for cross-sections being: σ s {\displaystyle \sigma _{s}} , σ γ {\displaystyle \sigma _{\gamma }} , σ a {\displaystyle \sigma _{a}} , etc. A special case is the total cross-section σ t {\displaystyle \sigma _{t}} , which gives the probability of a neutron to undergo any sort of reaction ( σ t = σ s + σ γ + σ f + … {\displaystyle \sigma _{t}=\sigma _{s}+\sigma _{\gamma }+\sigma _{f}+\ldots } ).
Formally, the equation above defines the macroscopic cross-section (for reaction x) as the proportionality constant between a particle flux incident on a (thin) piece of material and the number of reactions that occur (per unit volume) in that material. The distinction between macroscopic and microscopic cross-section is that the former is a property of a specific lump of material (with its density), while the latter is an intrinsic property of a type of nuclei.
Younes, Walid; Loveland, Walter (2021). An Introduction to Nuclear Fission. Springer. pp. 10, 25–26, 56–58. ISBN 9783030845940. 9783030845940 ↩
Rhodes, Richard (1986). The Making of the Atomic Bomb. New York: Simon & Schuster Paperbacks. pp. 333–334, 282–287. ISBN 9781451677614. 9781451677614 ↩