DISSERTATION
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_____________________________________________________________ Results and Discussion<br />
A similar result is observed for the pulse profile with 500 mV potential difference (Figure 3.22,<br />
yellow curve). Although the potential difference is higher than for the 0.5/0.2 V pulse profile,<br />
the applied negative potential is apparently not sufficiently low to induce effective enough ion<br />
stirring and push up already immobilized DNA strands that are lying on the surface as a random<br />
coil due to their low persistence length. Therefore, the access of new strands is hindered and a<br />
poor immobilization yield is observed. On the other hand, further increase of the potential<br />
difference to 700 mV (pulse profile 0.5/-0.2 V) leads to a significantly improved immobilization<br />
yield (Figure 3.22, green curve). Evidently, this pulse profile is vigorous enough to increase the<br />
ion flux and to induce improved ion stirring. Thus, already immobilized DNA strands can be<br />
lifted from the electrode surface and can create space for new strands to approach the surface.<br />
As explained earlier, even though for higher applied potentials the potential drop is steeper, at<br />
a certain distance from the electrode, the DNA is affected by an absolute higher potential.<br />
Figure 3.22. Comparison of different pulse profiles used for potential-assisted DNA<br />
immobilization. MCH-modified electrode was prepared as stated in Figure 3.8. ssDNA<br />
immobilization was performed for 15 min by incubation at OCP or using different pulse<br />
profiles (0.5/0.2 V, 0.5/0 V and 0.5/-0.2 V) with 10 ms pulse duration. MCH passivation<br />
and EIS measurements were performed as stated in Figures 3.7 and 3.8. Figure adapted<br />
from ref. 5 .<br />
3.3 Importance of controlling the surface 57