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______________________________________________________________________ Introduction<br />

1.2.2 DNA in front of a polarized electrode<br />

In addition to the DNA-ion interaction, it is important to understand the influence of a charged<br />

electrode on the behavior of DNA on its surface for the application in DNA sensing at electrified<br />

surfaces. The GC model of the double layer describes how the ionic strength and the<br />

polarization of the electrode influence the double layer structure and the potential drop in front<br />

of the electrode. The GC equation:<br />

Φ = 2kT<br />

e<br />

ln 1 + γexp ( −d<br />

κ −1)<br />

1 − γexp ( −d<br />

κ −1) (1.12)<br />

γ = tanh ( eΦ 0<br />

4kT ) (1.13)<br />

where Φ0 and Φ are the potentials at the electrode surface and at a distance d from the surface,<br />

respectively, reveals that the potential distribution strongly depends on the ionic strength, where<br />

an increase of the ionic strength leads to a steeper drop of the potential (Figure 1.7, a). Thus, a<br />

few nm away from the surface, Brownian motion prevails over electric forces and dominates<br />

the system response 42 . Furthermore, the model predicts a sharp potential drop for highly<br />

charged electrodes (high Φ0), while the decline is more gradual for lower Φ0 values 43 (Figure<br />

1.7, b).<br />

The DNA conformation on the electrode surface can be manipulated by externally applied<br />

potentials 44,45 . However, this is true only under certain conditions 42 . Namely, as in solutions of<br />

high ionic strength the applied potential decays within a nm distance, the range is too short to<br />

significantly affect grafted DNA molecules. Therefore, both negative and positive potentials do<br />

not affect the conformation of neither ds- nor ssDNA. dsDNA exhibits a rigid conformation,<br />

while ssDNA coils on the electrode surface (Figure 1.8, a). This remarkable difference in<br />

conformation originates from the difference in the persistence length of dsDNA and ssDNA, as<br />

explained in Section 1.2.1. Furthermore, in presence of filler molecules with height comparable<br />

to the length of the DNA spacer, the dsDNA conformation is almost perpendicular with respect<br />

to the electrode surface 42,45 . The reason for the upright conformation is the steric repulsion<br />

between the lowest base pairs and a monolayer that backfills the gold electrode between DNA<br />

strands. In contrast, ssDNA remains lying on the surface since, besides the very weak electrical<br />

interactions, self-repulsion along the DNA strand is suppressed by the high ionic strength.<br />

1.2 DNA 13

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