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. 2024 Feb 13;14:3628. doi: 10.1038/s41598-024-54343-y

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© The Author(s) 2024

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 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) Ratio of $Φ_{S}$ percentages, S plotted in the $k - r$ plane. The lighter yellow areas are closer in value to the ratios seen in Tables 1 and 2. (b) Variation of $Φ_{S}$ percentage with magnetic field strength ranging from 0.15 to 100 mT. The figure is plotted with $k = 2 \times 10^{6} s^{- 1}$ and $r = 1 \times 10^{6} s^{- 1}$ , which corresponds to $S = 1.24$ . All the figures are plotted considering the HFI contribution from the hydrogen atom of the Tyrosine oxyradical with the highest HFCC, $a_{A} = 1.86$ mT. We also consider the contribution of the ²⁵Mg isotope at its natural abundance of 10%. The HFI contribution from the same is $a_{B} = - 11.22$ mT.