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. 2023 Sep 11;30(10):1571–1581. doi: 10.1038/s41594-023-01093-6

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© The Author(s) 2023

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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Extended Data Fig. 4 — a). Heatmap representation of simulated S1 nucleosomal arrays generated through a Monte-Carlo simulation. Column 1 represents simulated ‘native’ arrays; Column 2 represents simulated ‘clamp’ remodeled arrays with a ruler length of 20 bp; Column 3 represents simulated ‘clamp’ remodeled arrays with a ruler length of 48 bp; Column 4 represents simulated ‘length-sensing’ remodeled arrays with a minimum flanking DNA length of 20 bp; Column 5 represents simulated ‘length-sensing’ remodeled arrays with a minimum flanking DNA length of 48 bp. b). The observation of density-dependent NRL scaling in ACF-remodeled products is neither impacted by ACF: mononucleosome stoichiometry (top) nor remodeling time (bottom).

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