FIG. 6.

Electric response (per unit cell) of L_y and S_y current influxes – $\Phi \left[Q_z^{L_y}\right]$ and $\Phi \left[Q_z^{S_y}\right]$ and various torques – $T_{\text{SO}}^{L_y}$, $T_{\text{CF}}^{L_y}$, $T_{\text{SO}}^{S_y}$, and $T_{\text{XC}}^{S_y}$ – arising from the interband processes and accumulation, and arising from the intraband processes (divided by τ) in Fe/W(110). Spatial profiles for (a) orbital and (b) spin quantities at the true Fermi energy $E_{\text{F}}=E_{\text{F}}^{\text{true}}$. Fermi energy dependence for (c) orbital and (d) spin quantities, summed over the ferromagnet layers (Fe1 and Fe2). Note that the sum of the interband responses of the orbital/spin current influx and the total torque ($T^{L_y}=T_{\text{SO}}^{L_y}+T_{\text{CF}}^{L_y}$ and $T^{S_y}=T_{\text{SO}}^{S_y}+T_{\text{XC}}^{S_y}$ for orbital and spin, respectively) matches with the intraband response of the orbital/spin accumulation divided by τ.