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Diplomarbeit Diplom-Ingenieur - Institut für Halbleiter

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38<br />

distribution is at about 30 nm and limited by 8 and 45 nm. If it is also taken into<br />

account that the dot elongation can be parallel to the line of sight, most of the dots in<br />

this sample are elongated. Unfortunately, no plan view specimen of this sample exists,<br />

but it should look like the plan view image of Figure 4.4, which shows an annealed<br />

3nm sample.<br />

Figure 4.7: (a) Height distribution of the dots. The maximum is at 25nm. The upper limit<br />

is at about 30nm. (b) Length distribution of the dots with the maximum at about 30nm.<br />

4.3.2 Annealed 1nm layer<br />

The same measurements were also performed for sample #28, with an originally 1nm<br />

thick PbTe layer. The sample was annealed at 320°C for 10 min. The plan view<br />

specimen of the sample was good enough for statistical evaluation. A cross sectional<br />

specimen was also available and was used to check the highly symmetric shape,<br />

which the dots show in the plan view sample. This can be seen in Figure 4.8. The<br />

appearance of the dots in plan view is an octagon with longer {110} interfaces. The<br />

distances between two parallel {110} interfaces were used to measure the size of the<br />

dots. The cross sectional specimen shows the appearance of these dots in a line of<br />

sight along the [ 110]<br />

direction which confirmed the high symmetry. One interesting<br />

point is the extended (111) interface of these small dots, which will be treated in part<br />

4.4.<br />

The distribution of the dot size can be seen in Figure 4.9. Figure 4.9a shows the<br />

high symmetry of the dots, which seem to become ever better for larger dots. The<br />

ideal case is again indicated with a solid line. The shift of the distribution to one side

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