Born approximation
The Born approximation is a way to estimate how a particle scatters off a target when the interaction between them is weak. It treats the scattering as a single, gentle nudge: the incoming wave passes through the target's potential, gets slightly deflected once, and travels on. The strong, repeated re-scattering that a strong potential would cause is simply neglected, which is exactly why the approximation is restricted to weak interactions.
Mechanically, it is the first term of a perturbation series for scattering. The pattern of where particles are deflected — the differential cross-section, telling us how likely each scattering angle is — comes out as essentially the strength of the potential measured at the particular change in momentum the particle undergoes. In clean language, the scattering pattern is a kind of transform of the potential's shape, so measuring how particles scatter at different angles maps out the structure of the target.
This makes the Born approximation a workhorse of scattering physics, from electrons probing atoms to neutrons mapping crystals to the analysis of particle collisions. It is honest about its domain: it holds when the scattering is weak — fast particles or feeble potentials — and it grows unreliable for slow particles, strong potentials, or resonances, where multiple scattering and the higher terms of the series can no longer be ignored.
The scattering amplitude is essentially a transform of the potential evaluated at the momentum transfer.
Being a first-order estimate, the Born approximation misses multiple scattering and resonances. It fails for strong potentials or slow particles, where higher terms or fully non-perturbative methods are required.