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. 2017 Jul 3;8:15928. doi: 10.1038/ncomms15928

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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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Simulations are consistent with γ=1.8 and inconsistent with mean-field theory. The signal has been averaged over avalanche realizations for durations T=40, 100, 105, 110, …, 200, 250 and the mean signal for each T is normalized so the area under the curve is unity before averaging over durations. Lines are fits using (7); fitted parameters are reported in Supplementary Table 2.

Inline graphic — Simulations are consistent with γ=1.8 and inconsistent with mean-field theory. The signal has been averaged over avalanche realizations for durations T=40, 100, 105, 110, …, 200, 250 and the mean signal for each T is normalized so the area under the curve is unity before averaging over durations. Lines are fits using (7); fitted parameters are reported in Supplementary Table 2.