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. 2020 Jul 28;34(2):249–260. doi: 10.1007/s10334-020-00868-y

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© The Author(s) 2020

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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Fig. 3 — Simulations results detailing the effects of variations in CEST framework conditions. Pulse durations t_p (100, 200, and 300 ms) (a), number of applied pulses n_p (n = 2 – 14) (b), and radiofrequency field strengths B₁ (0.2–1.4 µT) (c) were systematically varied. Each colored curve represents a simulated parameter value and gives the maximum magnetization transfer ratio asymmetry at different offset frequencies (0–4 ppm)