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                                   position of the tip as it is scanned across the surface. This mode of
                                   operation is usually preferred as it prevents the tip from crashing
                                   into the surface.
                                     During the STM experiment, when the tip is brought near the
                                   sample surface and the tunneling current is recorded, does it
                                   matter which way the tunneling electrons flow? How does the
                                   tunneling direction depend on the voltage bias applied to the sys-
                                   tem? To answer these questions, it is helpful to look at the energy
                                   band diagram for the tip-sample system. Figure 8.24(a) shows the
                                   energy band diagram for the STM tip and the sample separated
                                   by a small gap (vacuum or air barrier) without any voltage bias
                                   applied to the sample or the tip. Both the energy bands are typ-
                                   ical of a conductor where the electrons fill the energy levels up
                                   to the Fermi level, according to Pauli’s exclusion principle. With-
                                   out any voltage bias, the Fermi levels in the tip and sample are
                                   aligned, and there is no net electron-tunneling across the vacuum
                                   gap. Practical operation of the STM requires the application of
                                   a voltage bias across the tip and sample. When the STM tip is
                                   negatively biased (magnitude of the voltage bias is V) relative to
                                   the sample as depicted in Fig. 8.24(b), the energy levels of the tip
                                   is raised by an amount eV with respect to the energy levels of
                                   the sample. Hence, electrons from the tip within the band of eV
                                   from the Fermi level readily tunnel across the gap into the sam-
                                   ple. On the other hand, when the STM tip is positively biased
                                   relative to the sample, the reverse situation occurs as illustrated
                                   in Fig. 8.24(c), and electrons tunnel from the filled states in the
                                   sample to empty states in the tip. Thus the direction of flow of
                                   the tunneling electrons depends on the voltage bias adopted dur-
                                   ing the experiment. In addition, the magnitude of the measured
                                   current depends on the magnitude of the applied voltage bias.   ch08
                                     After the STM tip has completed imaging the sample surface
                                   under bias conditions, the computer program generates a false
                                   color image with little dots. Does this STM image represent the
                                   real positions of the individual atoms on the surface? It turns out
                                   that the answer to this question depends on the sample under
                                   investigation. Strictly speaking, the STM image represents the
                                   spatial variation of the electronic density at the surface. We may
                                   be “seeing” the atoms in some images, but not in others. We shall
                                   discuss a typical case of a semiconductor where care has to be
                                   taken in interpreting the image.
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