Electron spectra are generally presented in arbitrary units. The experimental elastic peak intensity I espec (E) is determined by the elastic backscattering probability I e (E) of electrons backscattered elastically within the solid angle of the spectrometer. The experimental elastic peak I espec (E) is converted to I e (E) backscattering probability using our new procedure based on the Goto i e (E) elastic backscattering current database. The elastic backscattering probability I c (E) was calculated applying the EPESWIN software of Jablonski. I e (E) < I c (E) due to the surface losses of electrons, characterized by the surface excitation parameter P se (SEP). P se (E) was determined experimentally using the Goto database and the relationship of Tanuma. Our new procedure is applied to angular-resolved (AREPES) spectra of Jablonski and Zemek presented in arbitrary units. In their AREPES experiments, the experimental elastic peak intensity I espec = I e (E, α d , ) was measured at α d angle of detection (35-74 • ) with a small HSA, with solid angle. The experimental value at 42• I e (E, 42 • , ) was converted to probability with the Goto database. It was corrected with a SEP parameter P se , determined by trial and error method for Si, Ni, Cu and Ag for E = 0.5 and 1 keV primary energies.