The use of synthetic DNA to design and build molecular machines and well-defined structures at the nanoscale has greatly impacted the field of nanotechnology. Here we expand the current toolkit in this field by demonstrating an efficient, quantitative, and versatile approach that allows us to remotely control DNA-based reactions and DNA nanostructure self-assembly using electronic inputs. To do so we have deposited onto the surface of disposable chips different DNA input strands that upon the application of a cathodic potential can be desorbed in a remote and controlled way and trigger DNA-based reactions and DNA nanostructure self-assembly. We demonstrate that this effect is specific and versatile and allows the orthogonal control of multiple reactions and multiple structures in the same solution. Moreover, the strategy is highly tunable and can be finely modulated by varying the cathodic potential, the period of applied potential, and the density of the DNA strand on the chip surface. Our approach thus represents a versatile way to remotely control DNA-based circuits and nanostructure assembly and can allow new possible applications of DNA-based nanotools.
Cooperativity enhances the responsiveness of biomolecular receptors to small changes in the concentration of their target ligand, albeit with a concomitant reduction in affinity. The binding midpoint of a two-site receptor with a Hill coefficient of 1.9, for example, must be at least 19 times higher than the dissociation constant of the higher affinity of its two binding sites. This trade-off can be overcome, however, by the extra binding energy provided by the addition of more binding sites, which can be used to achieve highly cooperative receptors that still retain high affinity. Exploring this experimentally, we have employed an “intrinsic disorder” mechanism to design two cooperative, three-binding-site receptors starting from a single-site—and thus noncooperative—doxorubicin-binding aptamer. The first receptor follows a binding energy landscape that partitions the energy provided by the additional binding event to favor affinity, achieving a Hill coefficient of 1.9 but affinity within a factor of 2 of the parent aptamer. The binding energy landscape of the second receptor, in contrast, partitions more of this energy toward cooperativity, achieving a Hill coefficient of 2.3, but at the cost of 4-fold poorer affinity than that of the parent aptamer. The switch between these two behaviors is driven primarily by the affinity of the receptors’ second binding event, which serves as an allosteric “gatekeeper” defining the extent to which the system is weighted toward higher cooperativity or higher affinity.
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