“…Our δV (q) does have this long wavelength limit but, contrary to the previous guess, is not monotonically increasing from q = 0 and eventually becomes positive when q is close to 2k F , k F being the Fermi wavenumber. When we revert to real space, δV (r) appears to be a sum of a number of Gaussian-like curves, which justifies the previous practice in electron energy band calculation, apparently based on experience and intuition [12,13]. However, appearance can be deceiving, for although the Gaussian curves can be a good starting point for band calculations, it is almost impossible to recover from them the desired (more realistic) δV (q) with the detail on which α 2 F (ν) sensitively depends [14].…”