Correction to “Slip Opacity and Fast Osmotic Transport of Hydrophobes at Aqueous Interfaces with Two-Dimensional Materials”

IF 15.8 1区 材料科学 Q1 CHEMISTRY, MULTIDISCIPLINARY ACS Nano Pub Date : 2024-11-24 DOI:10.1021/acsnano.4c14736
Maria Bilichenko, Marcella Iannuzzi, Gabriele Tocci
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Abstract

In the discussion of the results presented in Figure 4c of the originally published article, an error was introduced in describing the range of the diffusio-osmotic coefficient. Specifically, the following sentence incorrectly states the range as −450 μm2/s to +450 μm2/s, whereas the correct range is −4900 μm2/s to +5300 μm2/s, as shown in Figure 4c: “Notably, graphene-coated systems exhibit the largest variation in diffusio-osmotic mobility, ranging from approximately −450 μm2/s for bilayer graphene with r = 2.25 Å to around 450 μm2/s for single-layer graphene with r = 1.5 Å”. For all systems except those where graphene is in direct contact with water (i.e., the top two-dimensional material) DDO falls in a range between −1000 μm2/s and +1000 μm2/s. For systems where graphene is the top material instead, DDO can reach values approximately between −5000 μm2/s and +5000 μm2/s, depending on the size of the hydrophobic solute, further stressing the influence of the large slip-length of graphene on DDO, as opposed to systems where hBN or MoS2 are the top materials. In the original article, we discuss our numerical results in the broader context of diffusio-osmotic transport experiments on other systems, in particular on silica which can be considered a model system for studies of diffusio-osmosis. For example, the range of values of DDO reported in ref (1) (DDO = −230 μm2/s) and ref (2) (DDO = 200–800 μm2/s) is narrower than those on graphene-covered surfaces that we have investigated, highlighting the impact of slippage on diffusio-osmotic transport on graphene as opposed to a nonslipping surface such as silica. The conclusion of the manuscript regarding the influence of hydrophobes’ size and of the slip length on diffusio-osmotic transport is not altered by this correction, in fact we recognize that the slip-induced amplification of DDO is more pronounced than what we have discussed previously. We apologize for the error and any confusion it may have caused. This article references 2 other publications. This article has not yet been cited by other publications.
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二维材料水界面上憎水剂的滑动不透明度和快速渗透传输 "的更正
在讨论最初发表的文章图 4c 中的结果时,在描述扩散渗透系数的范围时出现了错误。具体来说,以下句子错误地将范围表述为 -450 μm2/s 至 +450 μm2/s,而正确的范围是 -4900 μm2/s 至 +5300 μm2/s,如图 4c 所示:"值得注意的是,石墨烯涂层系统的扩散渗透率变化最大,从 r = 2.25 Å 的双层石墨烯的约 -450 μm2/s 到 r = 1.5 Å 的单层石墨烯的约 450 μm2/s。除了石墨烯与水直接接触的系统(即最上面的二维材料)外,所有系统的 DDO 都在 -1000 μm2/s 和 +1000 μm2/s 之间。对于以石墨烯为顶层材料的系统,DDO 的值大约在 -5000 μm2/s 和 +5000 μm2/s 之间,具体取决于疏水性溶质的大小,这进一步强调了石墨烯的大滑移长度对 DDO 的影响,而不是以 hBN 或 MoS2 为顶层材料的系统。在原文中,我们结合其他体系的扩散渗流传输实验,特别是可视为扩散渗流研究模型体系的二氧化硅,讨论了我们的数值结果。例如,参考文献 (1) (DDO = -230 μm2/s)和参考文献 (2) (DDO = 200-800 μm2/s)中报告的 DDO 值范围比我们研究的石墨烯覆盖表面上的 DDO 值范围要窄,这突出说明了与二氧化硅等非滑动表面相比,滑动对石墨烯上的扩散渗透传输的影响。手稿中关于憎水体大小和滑移长度对扩散-渗透传输影响的结论并没有因为这一更正而改变,事实上,我们认识到滑移引起的 DDO 放大比我们之前讨论的更为明显。我们对这一错误及其可能造成的混淆表示歉意。本文引用了 2 篇其他出版物。本文尚未被其他出版物引用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
ACS Nano
ACS Nano 工程技术-材料科学:综合
CiteScore
26.00
自引率
4.10%
发文量
1627
审稿时长
1.7 months
期刊介绍: ACS Nano, published monthly, serves as an international forum for comprehensive articles on nanoscience and nanotechnology research at the intersections of chemistry, biology, materials science, physics, and engineering. The journal fosters communication among scientists in these communities, facilitating collaboration, new research opportunities, and advancements through discoveries. ACS Nano covers synthesis, assembly, characterization, theory, and simulation of nanostructures, nanobiotechnology, nanofabrication, methods and tools for nanoscience and nanotechnology, and self- and directed-assembly. Alongside original research articles, it offers thorough reviews, perspectives on cutting-edge research, and discussions envisioning the future of nanoscience and nanotechnology.
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