UCMR contribute to the total AMR, and it is difficult to separate these two contributions from each other; for $xz$-plane, the magnetic field is always perpendicular to the $\bf m$$_y$, $\bf m$$_y$ is the $y$ component of magnetization unit vector, the UCMR should remain constant, and any resistance change can be attributed to CMR; for $yz$-plane, the electrical current is always perpendicular to the magnetization, the CMR should remain constant, and only UCMR can be achieved. The PLL3 hybrid demonstrates clear UCMR below the Curie temperature of LCO film, with the amplitude exceeding 7 $\times$ 10$^{-5}$ \[see $\theta_{yz}$ scan in Fig. 10(a)\]; the $\theta_{xz}$ scans also show obvious CMR, indicating the existence of induced ferromagnetism at the Pt/LCO interface. Similar behaviors were also observed in Pd/YIG hybrid, where the amplitude of $\theta_{xz}$ scan increases as decreasing the temperature, as expected from the MPE induced ferromagnetism [@Lin2014]. However, at the temperatures above the $T_\textup{C}$ of LCO film, no MR oscillation can be found for all three field scans, and the resistance is almost independent of angle $\theta$, implying that the AMR observed in Pt/LCO hybrids is entangled with the ferromagnetism of LCO film. As shown in Fig. 10(b), the field dependence 