Nanopore unstacking of single-stranded DNA helices
Nanopore unstacking of single-stranded DNA helices
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DOI:
10.1002/smll.200700049
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发表时间:
2007-07-01
期刊:
影响因子:
13.3
通讯作者:
Li, Chang Ming
中科院分区:
文献类型:
--
作者:
Chen, Peng;Li, Chang Ming
The secondary structures and mechanical properties of nucleic acids play important roles in their functions as well as in relevant biological processes, such as DNA replication. Single-molecule force spectroscopy has emerged as a tool of unprecedented power for the study of molecular properties that are often obscured in ensemble-averaged macroscopic measurements.[1] A series of recent experimental and theoretical studies has demonstrated the utilization of voltagebiased nanometer-sized pores as a rapid single-molecule force spectroscope to sequentially unzip double-stranded (ds) DNAs, folded RNAs, or structured peptides and examine their properties and structures.[2–5] Most nanopore studies have relied on α-hemolysin, which self-assembles to form a protein channel with high fidelity across a lipid bilayer separating two ionic solution chambers. Imposition of a voltage bias across the nanopore establishes an ionic current and drives the translocation of charged biopolymers, such as DNAs, through the pore. Measurement of the transient reduction in the ionic current induced by this molecular translocation provides rich information regarding the properties of the translocated molecule as well as the dynamics of disrupting its structure as it is forced through the narrow aperture, which is barely larger than a nucleotide.[6–8] Here, we demonstrate the force-induced unstacking of individual single-stranded (ss) homopolymeric DNA helices during translocation through an α-hemolysin protein nanopore by electrophoresis. The unstacking energy and cooperativity are inferred from an analysis of the translocation kinetics.Studies of the translocation of ssDNA molecules through α-hemolysin pores have observed slow translocation kinetics rather than the expected rapid, free electrophoretic translocation.[6, 9] This anomalous behavior has been a topic of continuing speculation. The unexpectedly slow translocation of ssDNAs has been interpreted in terms of the free-energy barrier due to the conformational entropy of randomly coiled DNA molecules.[10] However, no such entropic effect has been observed in experiments involving the rapid electrophoretic transport of long dsDNA molecules through relatively large, fabricated, solid-state nanopores.[9, 11] Therefore, it has been proposed that the translocation kinetics is controlled by DNA–hemolysin interactions that retard the DNA motion, although the nature of such interactions still needs scrutiny.[12] Single-stranded homopolymeric nucleic acids have been shown to assume a rigid secondary helical structure that is stabilized by aromatic base stacking between consecutive bases along the sugar–phosphate backbone. X-ray scattering studies show that the helical diameters of RNA homopolymers polyA and polyC are about 2.1 and 1.9 nm, respectively,[13, 14] which are comparable to the diameter of the dsDNA helix (2.4 nm). The helical structures in ssDNA have also been identified experimentally [15–17] and theoretically.[18] Luzzati et al.[19] discovered an intermediate form of DNA, which may be a ssDNA in helical form and assumes an axial radius 70% of that of dsDNA. In support of this, by using