| Literature DB >> 32807877 |
Roman Zhuravel1, Haichao Huang1, Georgia Polycarpou2, Savvas Polydorides2, Phani Motamarri3,4, Liat Katrivas5, Dvir Rotem1, Joseph Sperling6, Linda A Zotti7,8, Alexander B Kotlyar5, Juan Carlos Cuevas7, Vikram Gavini3,9, Spiros S Skourtis2, Danny Porath10.
Abstract
Understanding charge transport in DNA molecules is a long-standing problem of fundamental importance across disciplines1,2. It is also of great technological interest due to DNA's ability to form versatile and complex programmable structures. Charge transport in DNA-based junctions has been reported using a wide variety of set-ups2-4, but experiments so far have yielded seemingly contradictory results that range from insulating5-8 or semiconducting9,10 to metallic-like behaviour11. As a result, the intrinsic charge transport mechanism in molecular junction set-ups is not well understood, which is mainly due to the lack of techniques to form reproducible and stable contacts with individual long DNA molecules. Here we report charge-transport measurements through single 30-nm-long double-stranded DNA (dsDNA) molecules with an experimental set-up that enables us to address individual molecules repeatedly and to measure the current-voltage characteristics from 5 K up to room temperature. Strikingly, we observed very high currents of tens of nanoamperes, which flowed through both homogeneous and non-homogeneous base-pair sequences. The currents are fairly temperature independent in the range 5-60 K and show a power-law decrease with temperature above 60 K, which is reminiscent of charge transport in organic crystals. Moreover, we show that the presence of even a single discontinuity ('nick') in both strands that compose the dsDNA leads to complete suppression of the current, which suggests that the backbones mediate the long-distance conduction in dsDNA, contrary to the common wisdom in DNA electronics2-4.Mesh:
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Year: 2020 PMID: 32807877 DOI: 10.1038/s41565-020-0741-2
Source DB: PubMed Journal: Nat Nanotechnol ISSN: 1748-3387 Impact factor: 39.213