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. 2018 Mar 20;9:1141. doi: 10.1038/s41467-018-03550-z

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© The Author(s) 2018

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. 4 — Monte Carlo Simulations of 2D superlattices of octapods with different pod length. a–d Snapshots showing a typical top-view configuration of the octapods at the end of our simulation run for different L/D. The value of the shaft interaction parameter ε_S and the tip interaction parameter ε_T are provided to the left of each snapshot, both are given in k_BT. A description of the crystal structure is given in the main text; the insets show a zoom-in to better visualize the structure. e Variation of the parameters ε_S and ε_T for octapods with L/D = 5.0 tune the octapod arrangement from ballerina (for ε_S = −3 and ε_T = 0) to interlocking (for ε_S = 2 and ε_T = −1). f The pressure was increased with respect to (a) and (c)