*.fet

Format Old format for earlier version

x y Ec Error n p Nda Impurity Efn Efp Traps generation Radiative non-radiative Auger temperature Ev uofEc uofEv uofEv2 Exciton region_num

new updated version (since 2023)

$x$ $y$ $Ec$ $Error$ $n$ $p$  $Nda$  $N_{imp}$  $E_{fn}$  $E_{fp}$  $Traps$    $Generation$  $R_{rad}$ $R_{nonrad}$ $R_{auger}$ $T$ $Ev$ $\frac{1}{u_{Ec,1}}$ $\frac{1}{u_{Ev,1}}$   $\frac{1}{u_{Ev,2}}$    $R_{Exciton}$    $Region_{ID}$    $\frac{1}{u_{Ec,2}}$    $Ec_{1,strained}$    $Ec_{2,strained}$    $Ev_{1,strained}$    $Ev_{2,strained}$    $n_{1st}$    $n_{2nd}$         $p_{hh,1st}$   $p_{lh,2nd}$   $R_{Rad,e-hh}$    $R_{Rad,e-lh}$

new updated version (since 2024.04)

$x$ $y$ $Ec$ $Error$ $n$ $p$  $Nda$  $N_{imp}$  $E_{fn}$  $E_{fp}$  $Traps$    $Generation$  $R_{rad}$ $R_{nonrad}$ $R_{auger}$ $T$ $Ev$ $\frac{1}{u_{Ec,1}}$ $\frac{1}{u_{Ev,1}}$   $\frac{1}{u_{Ev,2}}$    $R_{Exciton}$    $Region_{ID}$    $\frac{1}{u_{Ec,2}}$    $Ec_{1,strained}$    $Ec_{2,strained}$    $Ev_{1,strained}$    $Ev_{2,strained}$    $n_{1st}$    $n_{2nd}$         $p_{hh,1st}$   $p_{lh,2nd}$   $R_{Rad,e-hh}$    $R_{Rad,e-lh}$  $\int^{y_T}_{y_B} Jn_{x} dy$ $\int^{x_R}_{x_L} Jn_{y} dx$  $\int^{y_T}_{y_B} Jp_{x} dy$ $\int^{x_R}_{x_L} Jp_{y} dx$

$\int^{y_T}_{y_B} Jn_{x} dy$ Mean in each node point, the current flow in the x direction through at point is the integration from bottom neighbor point to the top neighbor point. The integration has a weighting of current from 0 (neighbor point) to 1 (node point) with FEM algorithm.

$\int^{x_R}_{x_L} Jn_{y} dx$ Mean in each node point, the current flow in the y direction through at point is the integration from left neighbor point to the right neighbor point. The integration has a weighting of current from 0 (neighbor point) to 1 (node point) with FEM algorithm.

Note that it is a integrated current density, not the current density. So it might have a larger current if the neighbor point is far away since the integration distance is longer.