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. 2020 Aug 14;13:145. doi: 10.1186/s13068-020-01782-0

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© The Author(s) 2020

Open AccessThis 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 licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence 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 licence, visit http://creativecommons.org/licenses/by/4.0/. The Creative Commons Public Domain Dedication waiver (http://creativecommons.org/publicdomain/zero/1.0/) applies to the data made available in this article, unless otherwise stated in a credit line to the data.

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Fig. 7 — Evaluation of the dynamical regime through non-linear normal mode analysis. Comparison between WTs Cs4130 and Gxf1 (a). The low-frequency mode 6 for Cs4130 and Gxf1 (with respective mutants) are shown in b and c, respectively. The displacement of the residues was evaluated using the root mean square fluctuation (RMSF)