「$Withionmove」：修訂間差異

於 2019年8月18日 (日) 03:01 的修訂

When the system has ion to perform as drift-diffusion equations, we solve the time dependent drift-diffusion for slow ion move simulation. Since the ion moves may not be governed fermi-level concept. We simply treat is a tradiational drift-diffusion equations.

 $\frac{\partial M_{i o n}}{\partial t} = \nabla ((q_{s i g n}) e μ M_{i o n} \vec{E} - q D_{M} \nabla M_{i o n})$

Ideally, the ion density is given by initial setting. The total ion number should be fixed. The program is aim to model multi-ions drift-diffusion. The command is as following.

$Withionmove
 $N_{s} w e e p$   $N_{o} u t p u t$ 
 $T_{1, s t o p}$    $d t_{1}$   $T_{2, s t o p}$    $d t_{2}$  ...  $T_{N_{s w e e p}, s t o p}$    $d T_{M_{s w e e p}}$ 
<math> N_{ions} ~~ q_{sign,1} ~~ q_{sign,2} ~~ q_{sign,3}  ....~~ q_{sign,N_{ions}}

@@ 第1行： / 第1行： @@
 When the system has ion to perform as drift-diffusion equations, we solve the time dependent drift-diffusion for slow ion move simulation. Since the ion moves may not be governed fermi-level concept. We simply treat is a tradiational drift-diffusion equations.
 <br>
-  <math> \frac{\partial M_{ion}}{\partial t} = \nabla \left( (\pm) e\mu M_{ion} \vec{E} - q D_{M} \nabla M_{ion} \right)</math>
+  <math> \frac{\partial M_{ion}}{\partial t} = \nabla \left( (q_{sign}) e\mu M_{ion} \vec{E} - q D_{M} \nabla M_{ion} \right)</math>
 Ideally, the ion density is given by initial setting. The total ion number should be fixed. The program is aim to model multi-ions drift-diffusion. The command is as following.
   $Withionmove
-  N_sweep N_output_per_step
+  <math> N_sweep </math> <math> N_output</math>
   <math>T_{1,stop}</math>  <math>dt_{1}</math> <math>T_{2,stop}</math>  <math>dt_{2}</math> ... <math>T_{N_{sweep},stop}</math>  <math>dT_{M_{sweep}}</math>
+ <math> N_{ions} ~~ q_{sign,1} ~~ q_{sign,2} ~~ q_{sign,3}  ....~~ q_{sign,N_{ions}}

「$Withionmove」：修訂間差異

於 2019年8月18日 (日) 03:01 的修訂

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