temperature and $R$ is the electron-phonon coupling constant. The solid lines through the data in Fig. 9 are fits to Eq. (4) and the fitting parameters are summarized in Table. I. The Debye temperatures $\Theta_R$ from the fit are much smaller than the value derived from electrical resistivity ($\Theta_R$ $\approx$ 240 K) and specific heat ($\Theta_D$ $\approx$ 225 K) of bulk Pt metal [@Meaden1969; @tari2003], again indicating the interfacial scattering contributes mostly to the electrical resistivity.

  ------- ------- ------ ------- --
                                 
  PLL2     0.215   5.76   157.5  
  PLLA2    0.294   6.08   153.0  
  PLS2     0.265   8.46   176.0  
  ------- ------- ------ ------- --

  : The values of $\rho_R$, $R$, and $\Theta_R$ derived from fittings to Eq. (4).[]{data-label="tab:table1"}

We also measure the angular and field dependence of MR for PLL and PLS hybrids. Both hybrids exhibit similar behaviors, for clarity, only the results of PLL hybrids are presented in Figs. 10 and 11. Figure 10 (a) plots the angular dependence of MR for Pt(3 nm)/LCO/LAO (PLL3) hybrid at 10 K and 100 K. The anisotropic magnetoresistance is defined as $\Delta$$\rho$/$\rho_0$ = \[$\rho$(M $\parallel$ I) - $\rho$(M $\perp$ I)\]/$\rho_0$, $\rho_0$ is zero field resistivity. According to Eq. (1), when magnetic field scans within $xy$-plane, both CMR and 