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. 2022 Apr 12;12:6109. doi: 10.1038/s41598-022-10068-4

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© The Author(s) 2022

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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The dependence of the triplet yield of the [ ${TrpH}^{. +} \dots O 2^{. -}$ ] complex on applied static magnetic field for $r = 10^{5}$ s $^{- 1}$ , $k = 10^{6}$ s $^{- 1}$ , $a_{A} = 1.6046$ mT. The triplet yield goes from around 60% to around 40% by changing the magnetic field strength from GMF to HMF. The strong HMF effect is further emphasized by the inset.