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. 2021 Feb 19;12:1212. doi: 10.1038/s41467-021-21234-z

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© The Author(s) 2021

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. 5 — a Mapping of temperature change ΔT as a function of the bias magnetic field μ₀H₀ and temperature. b Typical heat cycles when the magnetic field rises from each μ₀H₀ by Δμ₀H = 0.4 T. The inset shows a magnification of the most efficient cycle for μ₀H₀ = 0.5 T and T = 28.2 K.