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. 2020 Jun 4;11:2822. doi: 10.1038/s41467-020-15535-y

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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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Fig. 2 — The simulations are performed with different solvation timescales, τ_D, while fixing other parameters at J = 0.020 eV, ΔG^o = −0.60 eV, λ_i = 0.80 eV, and λ_o = 0.40 eV. It is assumed that excited-state (ES) global minimum is aligned with the ground state (GS) global minimum along the x coordinate. a Simulations using the nonergodic model. b Simulations using the Sumi-Marcus model. Note the difference in the variation of β between two models.