dependence of the MR for Pt (3 nm)/LCO/LAO hybrid for $\theta_{xy}$, $\theta_{xz}$, and $\theta_{yz}$ scans. The data were measured at 10 K (solid symbols) and 100 K (open symbols) in a field of $\mu_0$H = 40 KOe. The solid lines through the data are fits to (cosine)$^2$ with 90 degree phase shift. (b) The field dependence of longitudinal ($\rho_\parallel$) and transverse ($\rho_\textup{T}$) MR ratio for Pt (3 nm)/LCO/LAO hybrid measured at $T$ = 2 K.[]{data-label="fig10"}](Fig10.eps){width="3.2in"}

![(Color online) Angular dependence of MR for Pt/LCO/LAO hybrid with different Pt thickness for $\theta_{xy}$ (a), $\theta_{xz}$ (b), and $\theta_{yz}$ (c) scans. The data were measured at 10 K in a field of $\mu_0$H = 40 KOe, which is sufficiently strong to saturate the LCO magnetization.[]{data-label="fig11"}](Fig11.eps){width="3.2in"}

Figure 9 shows temperature dependence of the electrical resistivity for PLL2, PLLA2, and PLS2 hybrids. The electrical resistivity in all films increases linearly with temperature, exhibiting typical metallic behavior. The temperature dependence of the electrical resistivity can be well described by the Bloch-Grüneisen relation [@Meaden1969]: $$\rho(T) = \rho_R + \frac{4R}{\Theta_R}(\frac{T}{\Theta_R})^5\int_0^{\frac{\Theta_R}{T}}\frac{x^5}{(e^x-1)(1-e^{-x})}dx$$ where $\rho_R$ is the residual resistivity due to the static defects in the crystal lattice; second term represents the contribution of electron-phonon scattering, in which $\Theta_R$ is the Debye 