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Figure 3: The dependencies ² 00 (log !¿¾). The values are normalized at ² 00 max-TOWARD THE PHYSICAL BASIS OF COMPLEX SYSTEMS: DIELECTRIC ANALYSIS OF POROUS SILICON NANOCHANNELS IN THE ELECTRICAL DOUBLE LAYER LENGTH RANGE

<p>Fig.3. The conductivity relaxation occurs at<br> lowing frequencies. The form of the &sup2;<br> 00<br> (!) = f(&sup2;<br> 0<br> (!)) diagrams changes from<br> a vertical line (a), to any deformate semicircles (b, c, d) having the angle to<br> real axe below &frac14;<br> 2 , Fig.4. This behaviour denotes that the EDL is not an ideally<br> capacitor, but also is not a disipative region, depending both on the EDL<br> thickness and the frequency range of the applied &macr;eld [7]. The composition<br> (by thickness) of the EDL determines essentially the dielectric response of the<br> interface system. Compared with experimental results, the dielectric pro&macr;le<br> of this higher length scales model, can provides a more complet description of<br> the solvent properties for a given electrode.</p>

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40/100

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8
Harmonization
4
Access
20
Reuse readiness
8
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