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Results and Discussion<br />

of the Rct. Moreover, the presence of additional DNA strands leads to an additional steric<br />

hindrance decreasing the access of the redox mediator and contributes to an increase in Rct with<br />

a strong dependence on ssDNA coverage. When the coverage is very low, additional DNA<br />

strands do not notably alter the surface architecture and the redox mediator access is negligibly<br />

hampered. At high ssDNA coverage which is however low enough to allow for maximum<br />

hybridization efficiency, the approach of the redox mediator to the electrode surface is more<br />

likely affected.<br />

Nevertheless, due to the low persistence length of ssDNA it behaves as random coil lying on<br />

top of the thiol passivation layer (Figure 3.10) still preventing the access of the redox mediator<br />

to the electrode surface. The structure of the formed dsDNA is more rigid as compared to the<br />

one of the ssDNA, leading to a more upright orientation of the dsDNA and facilitating the<br />

approach of the redox species. The degree of this influence depends on the length of DNA<br />

strands. Short DNA is expected to exhibit only a little impact while longer DNA causes a more<br />

significant change of the electrode architecture.<br />

Figure 3.10. Interfacial changes upon DNA hybridization. DNA obtains a more upright<br />

orientation due to the rigidity of the dsDNA. Furthermore, the amount of the negative<br />

charge increases and an additional steric hindrance arises due to an increased number of<br />

strands. Thiol passivation layer was intentionally not shown for better clarity.<br />

3.2 Importance of knowing the surface 40

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