"$usemunpfunc" 修訂間的差異
出自 DDCC TCAD TOOL Manual
| (未顯示由 1 位使用者於中間所作的 1 次修訂) | |||
| 行 43： | 行 43： | ||
<math>\mu_{n,temp}=\mu_0 exp(\beta\sqrt{E})</math>, <math>\mu_{p,temp}=\mu_0 exp(\beta\sqrt{E})</math> |
<math>\mu_{n,temp}=\mu_0 exp(\beta\sqrt{E})</math>, <math>\mu_{p,temp}=\mu_0 exp(\beta\sqrt{E})</math> |
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| − | If <math> \mu_{n,temp} \times E > v_{n,sat}, then |
+ | If <math> \mu_{n,temp} \times E > v_{n,sat}, then \mu_n = \frac{v_{n,sat}}{E} </math> |
| − | If <math> \mu_{ |
+ | If <math> \mu_{p,temp} \times E > v_{p,sat}, then \mu_p = \frac{v_{p,sat}}{E} </math> |
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| + | <big>'''The $usemunpfunc setting for 1D-DDCC in GUI interface '''</big> <br> |
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| + | The parameters are modified in step 4.<br> |
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| + | [[檔案:1d_$usemunpfunc_fig1.jpg|1300px]]<br> |
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| + | [[檔案:1d_$usemunpfunc_fig2.jpg|300px]]<br> |
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於 2025年1月6日 (一) 19:36 的最新修訂
Function for organic material. We usually assume the carrier mobility is depend on electrical field and follow Poole-Frenkel field dependent mobility equation.
Mobility follow this equation
Where
-
is the zero-field mobility -
is the factor of mobility increasing -
is the electric field.
Format
$usemunpfunc 1 μe βe μh βh
Parameter Explanation
,
- μe : electron zero-field mobility.
- βe : electron beta.
- μh : hole zero-field mobility.
- βh : hole beta.
$usemunpfunc 11 μe βe μh βh
Parameter Explanation
- μe : electron zero-field mobility.
- βe : electron beta.
- μh : hole zero-field mobility.
- βh : hole beta.
- saturate electron velocity (cm/s)
- saturate hole velocity (cm/s)
,
IfIf
The $usemunpfunc setting for 1D-DDCC in GUI interface
The parameters are modified in step 4.
