Figure 3.

Induced electron density (a) and the total electrostatic potential (b) in response to small atomic displacements in the three crystalline bulk test cases: diamond silicon, NaCl and copper perfect crystals. A single Si, Na, Cl or Si is displaced in a random direction by 0.1 Å. The average of the induced electron density or potential is calculated over thin spherical shells of radius x centered at the original position of the displaced atom. Note that all atoms are equivalent thanks to the translational symmetry of the crystal. The trends \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$x^{-1}$$\end{document} and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$x^{-3}$$\end{document} and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$x^{-1}\exp (-x/r_s)$$\end{document} are indicated by thin lines to help the eye. In (b), the screening length is arbitrarily set to \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$r_s=4$$\end{document} Å.