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(100) orientation relative to that of the (111) orientation. 2,38 Figure 8.3 shows i-V curves
of different types of Si in 1% HF solution. Except for a shift along the potential axis,
which reflects the difference in the Fermi levels of these materials, the i-V curves
of
p
type and heavily doped n types are largely identical.
The i-V curves on non-heavily doped n -Si are shown in Fig. 8.4. Unlike p
and
heavily doped n -Si, a much larger anodic polarization is required to generate the dis-
solution reaction in the dark; the lower the doping level, the higher the applied poten-
tial for a given current density. 2 Also, the i-V curves may not show the clearly defined
regions as on other types of Si, but depend on measurement procedures. As shown in
Fig. 8.4 the i-V curve with a positive potential scanning rate is different from that with
a negative scanning rate; different regions are revealed only on the curve measured at
a certain negative scanning rate. As will be discussed later, it is the particular reaction
and the morphology that give rise to the i-V characteristics shown in Fig. 8.4. Also,
the current flow on n -Si is very sensitive to surface roughness. 9,42 Mechanical
-Si
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