How local is the Phantom Force?
  The phantom force is an apparently repulsive force, which can dominate the atomic contrast of an AFM image when a tunneling current is present. We described this effect with a simple resistive model, in which the tunneling current causes a voltage drop at the sample area underneath the probe tip. Because tunneling is a highly local process, the areal current density is quite high, which leads to an appreciable local voltage drop that in turn changes the electrostatic attraction between tip and sample. However, Si(111)-7\times7 has a metallic surface-state and it might be proposed that electrons should instead propagate along the surface-state, as through a thin metal film on a semiconducting surface, before propagating into the bulk. In this article, we investigate the role of the metallic surface-state on the phantom force. First, we show that the phantom force can be observed on H/Si(100), a surface without a metallic surface-state. Furthermore, we investigate the influence of the surface-state on our phantom force observations of Si(111)-7\times7 by analyzing the influence of the macroscopic tip radius R on the strength of the phantom force, where a noticeable effect would be expected if the local voltage drop would reach extensions comparable to the tip radius. We conclude that a metallic surface-state does not suppress the phantom force, but that the local resistance Rs has a strong effect on the magnitude of the phantom force. 
Thorsten Wutscher, Alfred J. Weymouth and Franz J. Giessibl
cond-mat.mtrl-sci