Effective collision strength

The effective collision strength is the dimensionless thermal average of an electron-impact collision strength. For a Maxwellian electron population, with collision energy $E$ measured above the upper-level threshold,It is a function of temperature, rather than a cross section evaluated at one representative energy.

If $\Omega$ is constant, the normalized exponential weight gives ${\rm Y}=\Omega$. Near-threshold resonances can instead strongly change the average, particularly at low temperature. Atomic excitation and de-excitation rate coefficients use this average together with statistical weights and, for excitation, the appropriate Boltzmann threshold factor.^[ref]