The model [1] consists of two modules: (a) bulk and (b) FMI|NM interface modules. The bulk module, which is a π - model, takes into account the pure spin (longitudinal to the magnetization direction) transport by magnon diffusion. The series conductance takes into account the spin transmission from one surface to the other, while the shunt conductances take into account the spin relaxation. The series conductance has the interface conductance for the spins that are longitudinal to the magnetization direction. The shunt conductance captures the spin relaxation for transverse spins at the interface. The interface module is similar to already existing FM|NM module except the charge conductance is negligible compared to the spin conductance since FMI is an insulator. The models are shown below:
with the following conductances matrices in c-z-x-y basis where c is charge and z, x, y are spin polarization.
Parameter | Symbol | Unit |
Pure Spin Resistivity | ||
Magnon Diffusion Length | ||
Length | ||
Cross-Sectional Area | ||
Interface Spin Conductance (Longitudinal Spins) | ||
Real Part of Spin Mixing Conductance (Transverse Spins) | ||
Imaginary Part of Spin Mixing Conductance (Transverse Spins) |
The module, as a part of the library, can be downloaded here.
Please contact Shehrin Sayed ( ssayed AT berkeley DOT edu or ssayed AT lbl DOT gov) for questions or comments regarding this page.
[1] S. Sayed, V. Q. Diep, K. Y. Camsari, and S. Datta, "Spin Funneling for Enhanced Spin Injection into Ferromagnets". Scientific Reports, 6: 28868 (2016). (Link).