Quantitative low-energy electron diffraction LEED I(V) or LEED I(E), which evaluates the diffraction intensities I as a function of the electron energy, is a versatile technique for the study of surface structures. The technique is based on optimizing the agreement between experimental and calculated intensities. Today, the most commonly used measure of agreement is Pendry's RP. While RPhas many advantages it also has severe shortcomings, as it is a noisy target function for optimization and very sensitive to small offsets of the intensity. Furthermore, RP= 0, which is meant to imply perfect agreement between two I(E) curves, can also be achieved by qualitatively very different curves. We present a modified RS, which can be used as a direct replacement for RP, but avoids these shortcomings. We also demonstrate that RSis as good as RPor better in steering the optimization to the correct result in the case of imperfections in the experimental data, while another common R factor, RZJ(suggested by Zanazzi and Jona) is worse in this respect.
Imre et al. (Thu,) studied this question.