檢視 *.fet 的原始碼


<big><big>'''Format'''</big></big>   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)

 <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.

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.