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. 2022 Jan 12;13:278. doi: 10.1038/s41467-021-27861-w

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© The Author(s) 2022

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.

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Fig. 3 — A Electrostatic boundary condition including potential set for cathode (ground at S@C, conventional sulfur in carbon) and anode (2 V at Li, Lithium metal), and surface charged density (σ) on ANF wall. B Boundary condition for ion transport module for LPS anion and Li cation. The concentration map and streamline change (from t = 0 to t = 1 μs) of Li cation (C) and LPS anion (D) with (i) and without (ii) surface charge density on boundary of np-ANF separator.