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. 2020 Oct 19;10:17620. doi: 10.1038/s41598-020-73873-9

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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/.

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(A, B) Previously published data⁵ (exp. wg165) in which LCM and displacement were measured using a dual pressure-voltage sensor. All quantities are referenced to EC pressure. (A) Magnitude of LCM (thin) and BM displacement (thick). (B) Phase of LCM (thin) and BM displacement (thick). (C, D) Here LCM from wg165 are plotted with displacement found with a laser-based method (exp. GB800). These panels are included to reinforce the findings of (A, B). (C) Magnitude of LCM (thin) and BM displacement (thick). (D) Phase of LCM (thin) and BM displacement (thick). Positive displacement direction is up in Fig. 1, in the direction of the scala media. (Note: In the simultaneously gathered data of (A) and (B), a peak at $\sim$ 0.4 CF and dip at $\sim$ 0.5 CF are apparent in both displacement and LCM. Such a feature is not generally present; it might be due to a sound calibration or middle ear resonance in this preparation).