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. 2017 Jun 19;8:15863. doi: 10.1038/ncomms15863

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Copyright © 2017, The Author(s)

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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(a) Numerical solution of the model showing an expanding wavefront that reverses propagation direction at the boundary and closes back to a point. The results are plotted in terms of the experimental observable F+B. (b and c) Cross sections in normal direction to the expanding/contracting wavefronts at t=69 and t=220, respectively. The peak in the B field corresponds to the wavefront of CDRs. Note the pronounced depletion of F in the area surrounded by the wavefront.