Sequence Dependence of Charge Transport Properties of DNA

The electrical conduction through three short oligomers (26 base pairs, 8 nm long) with differing numbers of GC base pairs was measured. One strand is poly(A)−poly(T), which is entirely devoid of GC base pairs. Of the two additional strands, one contains 8 and the other 14 GC base pairs. The oligome...

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Bibliographic Details
Published inThe journal of physical chemistry. B Vol. 110; no. 18; pp. 8910 - 8913
Main Authors Nogues, C, Cohen, S. R, Daube, S, Apter, N, Naaman, R
Format Journal Article
LanguageEnglish
Published United States American Chemical Society 11.05.2006
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Summary:The electrical conduction through three short oligomers (26 base pairs, 8 nm long) with differing numbers of GC base pairs was measured. One strand is poly(A)−poly(T), which is entirely devoid of GC base pairs. Of the two additional strands, one contains 8 and the other 14 GC base pairs. The oligomers were adsorbed on a gold substrate on one side and to a gold nanoparticle on the other side. Conducting atomic force microscope was used for obtaining the current versus voltage curves. We found that in all cases the DNA behaves as a wide band-gap semiconductor, with width depending on the number of GC base pairs. As this number increases, the band-gap narrows. For applied voltages exceeding the band-gap, the current density rises dramatically. The rise becomes sharper with increasing number of GC base pairs, reaching more than 1 nA/nm2 for the oligomer containing 14 GC pairs.
Bibliography:istex:8CC82644CE8329DE5730BD8281F7184E0B0998AE
ark:/67375/TPS-C1QSPFJH-H
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ISSN:1520-6106
1520-5207
DOI:10.1021/jp060870o