"*.fet" 修訂間的差異

於 2024年4月7日 (日) 16:42 的最新修訂

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: This 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.

@@ 行 16： / 行 16： @@
 <math>\int^{y_T}_{y_B} Jn_{x} dy</math>  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.
-<math>\int^{x_R}_{x_L} Jn_{y} dx</math>  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.
+<math>\int^{x_R}_{x_L} Jn_{y} dx</math>  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. <br>
 '''Note:''' This 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.

"*.fet" 修訂間的差異

於 2024年4月7日 (日) 16:42 的最新修訂

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