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. 2020 Feb 14;10:2628. doi: 10.1038/s41598-020-59575-2

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© The Author(s) 2020

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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Survival function of the ORL emission. Survival function $S (I)$ pooled across wavelengths for pump fluences (a) 333.71 mJ/cm², (b) 460.49 mJ/cm², (c) 552.94 mJ/cm², and (d) 774.16 mJ/cm². Orange curve is obtained from the intensities pooled across wavelengths after normalizing by their corresponding shot-averaged value at each wavelength, while the blue curve is obtained from the intensities pooled across the wavelengths and shots before normalizing by their average value. A power-law line (green curve) with exponent −1 is shown for reference. (e,f) Sample emission spectrum and (g,h) lasing mode survival functions of the ORL at pump fluences: (e,g) 333.71 mJ/cm² and (f,h) 552.94 mJ/cm². Survival functions of the lasing modes show faster than the exponential decay due gain saturation in the ORL.