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. 2018 Aug 7;9:3118. doi: 10.1038/s41467-018-05611-9

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© The Author(s) 2018

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. 6 — Dependence of the spin Hall conductivity on the resistivity of Pt. Purple filled circles show the spin Hall conductivity (SHC) calculated from the experimentally measured spin–charge conversion current I_ISHE, assuming A′ = 0.05 nA Ω cm; blue filled circles show SHC σ_SH from the band calculations of Kontani et al.⁴⁴. The experimentally measured decrease of SHC follows the theoretically predicted ρ⁻² dependence of the SHC in the high-resistivity regime (dashed blue line)^8,44. The SHC values are given in ℏ/e units