Sahu Subin, Zwolak Michael
Biophysical and Biomedical Measurement Group, Microsystems and Nanotechnology Division, Physical Measurement Laboratory, National Institute of Standards and Technology, Gaithersburg, MD 20899, USA.
Institute for Research in Electronics and Applied Physics and Maryland NanoCenter, University of Maryland, College Park, MD 20742, USA.
Entropy (Basel). 2020 Nov 20;22(11):1326. doi: 10.3390/e22111326.
Ionic transport in nano- to sub-nano-scale pores is highly dependent on translocation barriers and potential wells. These features in the free-energy landscape are primarily the result of ion dehydration and electrostatic interactions. For pores in atomically thin membranes, such as graphene, other factors come into play. Ion dynamics both inside and outside the geometric volume of the pore can be critical in determining the transport properties of the channel due to several commensurate length scales, such as the effective membrane thickness, radii of the first and the second hydration layers, pore radius, and Debye length. In particular, for biomimetic pores, such as the graphene crown ether we examine here, there are regimes where transport is highly sensitive to the pore size due to the interplay of dehydration and interaction with pore charge. Picometer changes in the size, e.g., due to a minute strain, can lead to a large change in conductance. Outside of these regimes, the small pore size itself gives a large resistance, even when electrostatic factors and dehydration compensate each other to give a relatively flat-e.g., near barrierless-free energy landscape. The permeability, though, can still be large and ions will translocate rapidly after they arrive within the capture radius of the pore. This, in turn, leads to diffusion and drift effects dominating the conductance. The current thus plateaus and becomes effectively independent of pore-free energy characteristics. Measurement of this effect will give an estimate of the magnitude of kinetically limiting features, and experimentally constrain the local electromechanical conditions.
纳米至亚纳米尺度孔隙中的离子传输高度依赖于转运屏障和势阱。自由能景观中的这些特征主要是离子脱水和静电相互作用的结果。对于原子级薄膜中的孔隙,如石墨烯,其他因素也会起作用。由于几个相当的长度尺度,如有效膜厚度、第一和第二水化层半径、孔隙半径和德拜长度,孔隙几何体积内外的离子动力学在决定通道的传输特性方面可能至关重要。特别是对于仿生孔隙,如我们在此研究的石墨烯冠醚,由于脱水和与孔隙电荷相互作用的相互作用,存在传输对孔径高度敏感的区域。例如,由于微小应变导致的皮米级尺寸变化可导致电导率发生很大变化。在这些区域之外,即使静电因素和脱水相互补偿以给出相对平坦的——例如,接近无势垒的自由能景观,小孔径本身也会产生很大的电阻。然而,渗透率仍然可能很大,离子在到达孔隙的捕获半径内后将迅速转运。这反过来又导致扩散和漂移效应主导电导率。因此,电流趋于平稳并实际上变得与孔隙自由能特征无关。对这种效应的测量将给出动力学限制特征大小的估计,并通过实验限制局部机电条件。