Fig. 5: Electron transport and magnetization reversal of the MOS.
From: Unlocking property constraints through a multi-level ordered structure strategy

a Experimental temperature rise curves (left) and temperature distribution images (right) of the MOS, HS, and the state-of-the-art commercial SmCo5, Sm2Co17, and NdFeB in an alternating magnetic field. b Experimental data and model fitting of temperature-dependent electrical resistivity of the MOS. c Electrical resistivity enhancement along gradient direction of the MOS. d Four models in the simulations represent single-phase NdFeB (SP), NdFeB/α-Fe composite (COM), NdFeB/α-Fe composite with core-shell (CS) structure, and MOS sandwich core-shell (SCS) structure. e Electrical resistivity calculated by simulations with different models, as well as the corresponding resistivity measured in single-phase NdFeB (represents SP), Nd2Fe14B/α-Fe prepared by melt spinning (represents COM), surface of the GS Nd2Fe14B/α-Fe with a core-shell structure (represents CS), and surface of the MOS (represents SCS). f Initial magnetization curves (left) and their corresponding differential curves (right) of the MOS and HS. g Applied field dependence of Hc (left) for the MOS and HS, along with their corresponding differential curves (right) of the MOS and HS. The primary pinning field Hp is indicated in (f) and (g).