Abstract
An efficient iterative technique is presented for solving the Fredholm integral equation of the first kind, h(x) = ∫abdx′ g(x, x′)f(x′) , which occurs in various forms in experimental intensity measurements; h is the measured intensity distribution, f is the ideal distribution, and g is a bandpass function representing apparatus resolution. The scheme is based on the equations f0(x) = h(x) and fn+1(x) = fn(x)[h(x)/∫dx′g(x, x′)fn(x′)] and is shown to result in a nonnegative distribution free of diffraction effects. The method is easily extended to multidimensional abscissas x and multidimensional integrals, and an application to molecular beam data reduction for doubly differential reaction cross sections is presented.