「*.fet」：修訂間差異

於 2024年4月7日 (日) 08:42 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)

 $x$   $y$   $E c$   $E r r o r$   $n$   $p$    $N d a$    $N_{i m p}$    $E_{f n}$    $E_{f p}$    $T r a p s$      $G e n e r a t i o n$    $R_{r a d}$   $R_{n o n r a d}$   $R_{a u g e r}$   $T$   $E v$   $\frac{1}{u_{E c, 1}}$   $\frac{1}{u_{E v, 1}}$     $\frac{1}{u_{E v, 2}}$      $R_{E x c i t o n}$      $R e g i o n_{I D}$      $\frac{1}{u_{E c, 2}}$      $E c_{1, s t r a i n e d}$      $E c_{2, s t r a i n e d}$      $E v_{1, s t r a i n e d}$      $E v_{2, s t r a i n e d}$      $n_{1 s t}$      $n_{2 n d}$           $p_{h h, 1 s t}$     $p_{l h, 2 n d}$     $R_{R a d, e - h h}$      $R_{R a d, e - l h}$

new updated version (since 2024.04)

 $x$   $y$   $E c$   $E r r o r$   $n$   $p$    $N d a$    $N_{i m p}$    $E_{f n}$    $E_{f p}$    $T r a p s$      $G e n e r a t i o n$    $R_{r a d}$   $R_{n o n r a d}$   $R_{a u g e r}$   $T$   $E v$   $\frac{1}{u_{E c, 1}}$   $\frac{1}{u_{E v, 1}}$     $\frac{1}{u_{E v, 2}}$      $R_{E x c i t o n}$      $R e g i o n_{I D}$      $\frac{1}{u_{E c, 2}}$      $E c_{1, s t r a i n e d}$      $E c_{2, s t r a i n e d}$      $E v_{1, s t r a i n e d}$      $E v_{2, s t r a i n e d}$      $n_{1 s t}$      $n_{2 n d}$           $p_{h h, 1 s t}$     $p_{l h, 2 n d}$     $R_{R a d, e - h h}$      $R_{R a d, e - l h}$    $\int_{y_{B}}^{y_{T}} J n_{x} d y$   $\int_{x_{L}}^{x_{R}} J n_{y} d x$    $\int_{y_{B}}^{y_{T}} J p_{x} d y$   $\int_{x_{L}}^{x_{R}} J p_{y} d x$

$\int_{y_{B}}^{y_{T}} J n_{x} d y$ 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.

$\int_{x_{L}}^{x_{R}} J n_{y} d x$ 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.

@@ 第7行： / 第7行： @@
 new updated version (since 2023)
-<math> x</math> <math> y</math> <math> Ec</math> <math> Error</math> <math> n</math> <math> p </math>  <math>Nda</math>  <math> N_{imp}</math>  <math> E_{fn}</math>  <math> E_{fp} </math>  <math>Traps</math>    <math> Generation </math>  <math>R_{rad}</math> <math>R_{nonrad}</math> <math>R_{auger}</math> <math> T</math> <math>Ev </math> <math>\frac{1}{u_{Ec,1}}</math> <math>\frac{1}{u_{Ev,1}}</math> <math>\frac{1}{u_{Ev,2}}</math> <math> R_{Exciton}</math> <math>R_{ID} </math> <math>\frac{1}{u_{Ec,2}}</math> <math>Ec_{1,strained}</math>  <math>Ec_{2,strained}</math> <math>Ev_{1,strained}</math> <math>Ev_{2,strained}</math> <math>n_{1st}</math> <math>n_{2nd}</math> <math>p_{hh,1st}</math> <math>p_{lh,2nd}</math> <math>R_{Rad,e-hh}</math>  <math>R_{Rad,e-lh}</math>
+ <math> x</math> <math> y</math> <math> Ec</math> <math> Error</math> <math> n</math> <math> p </math>  <math>Nda</math>  <math> N_{imp}</math>  <math> E_{fn}</math>  <math> E_{fp} </math>  <math>Traps</math>    <math> Generation </math>  <math>R_{rad}</math> <math>R_{nonrad}</math> <math>R_{auger}</math> <math> T</math> <math>Ev </math> <math>\frac{1}{u_{Ec,1}}</math> <math>\frac{1}{u_{Ev,1}}</math>   <math>\frac{1}{u_{Ev,2}}</math>    <math> R_{Exciton}</math>    <math>Region_{ID} </math>    <math>\frac{1}{u_{Ec,2}}</math>    <math>Ec_{1,strained}</math>    <math>Ec_{2,strained}</math>    <math>Ev_{1,strained}</math>    <math>Ev_{2,strained}</math>    <math>n_{1st}</math>    <math>n_{2nd}</math>         <math>p_{hh,1st}</math>   <math>p_{lh,2nd}</math>   <math>R_{Rad,e-hh}</math>    <math>R_{Rad,e-lh}</math>
+new updated version (since 2024.04)
+ <math> x</math> <math> y</math> <math> Ec</math> <math> Error</math> <math> n</math> <math> p </math>  <math>Nda</math>  <math> N_{imp}</math>  <math> E_{fn}</math>  <math> E_{fp} </math>  <math>Traps</math>    <math> Generation </math>  <math>R_{rad}</math> <math>R_{nonrad}</math> <math>R_{auger}</math> <math> T</math> <math>Ev </math> <math>\frac{1}{u_{Ec,1}}</math> <math>\frac{1}{u_{Ev,1}}</math>   <math>\frac{1}{u_{Ev,2}}</math>    <math> R_{Exciton}</math>    <math>Region_{ID} </math>    <math>\frac{1}{u_{Ec,2}}</math>    <math>Ec_{1,strained}</math>    <math>Ec_{2,strained}</math>    <math>Ev_{1,strained}</math>    <math>Ev_{2,strained}</math>    <math>n_{1st}</math>    <math>n_{2nd}</math>         <math>p_{hh,1st}</math>   <math>p_{lh,2nd}</math>   <math>R_{Rad,e-hh}</math>    <math>R_{Rad,e-lh}</math>  <math>\int^{y_T}_{y_B} Jn_{x} dy</math> <math>\int^{x_R}_{x_L} Jn_{y} dx</math>  <math>\int^{y_T}_{y_B} Jp_{x} dy</math> <math>\int^{x_R}_{x_L} Jp_{y} dx</math>
+<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. <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」：修訂間差異

於 2024年4月7日 (日) 08:42 的最新修訂

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