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. 2019 Feb 11;9:1783. doi: 10.1038/s41598-018-38183-1

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© The Author(s) 2019

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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Simulated influence of the saturable absorber position. (a) Dynamic regimes of the tapered laser where Q-switched mode-locking (QSML), fundamental mode-locking (FML), unstable FML (uFML), third-order harmonic mode-locking (HML3), unstable HML3 (uHML3), asymmetric two-pulse mode-locking (A2P) and unstable A2P (uA2P) are observed. (b) Space-time diagram of A2P at the parameter point indicated with [b] in (a). The black vertical line in (a) indicates a 1D cut, for which peak power (red) and pulse width (blue) are shown in (c) and amplitude (black) and timing jitter (blue) are shown in (d).