"$usemunpfunc" 修訂間的差異
出自 DDCC TCAD TOOL Manual
Jameshuang (對話 | 貢獻) |
Jameshuang (對話 | 貢獻) |
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| 行 19： | 行 19： | ||
'''<big><big>Parameter Explanation</big></big>''' |
'''<big><big>Parameter Explanation</big></big>''' |
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| − | * μe : electron zero-field mobility <math>(cm^{2}eV^{-1}s^{-1})</math> |
+ | * μe : electron zero-field mobility. <math>(cm^{2}eV^{-1}s^{-1})</math> |
| − | * βe : electron beta <math>(eV^{-1/2})</math> |
+ | * βe : electron beta. <math>(eV^{-1/2})</math> |
| − | * μh : hole zero-field mobility <math>(cm^{2}eV^{-1}s^{-1})</math> |
+ | * μh : hole zero-field mobility. <math>(cm^{2}eV^{-1}s^{-1})</math> |
| − | * βh : hole beta <math>(eV^{-1/2})</math> |
+ | * βh : hole beta. <math>(eV^{-1/2})</math> |
於 2017年8月15日 (二) 16:53 的修訂
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.
