FIG. 14C illustrates the detailed temperature dependence of HIC from RT down to 11 K. It shows a nontrivial dependence that is not reflected by any of the models of IC described previously and does not match previous experimental data from other MTJ systems. Similarly, it does not follow the smooth temperature dependence of the switching field as shown in the inset of FIG. 14C, further confirming that it is not following the trend of the sample's PMA. In addition to the large magnitude and sign change shown between RT and 11 K in FIGS. 14A and 14B, there is a complex temperature dependence at intermediate temperatures, including multiple switches between AFM and FM coupling states, as shown in FIG. 14C.