「$usemunpfunc」：修訂間差異

於 2017年8月15日 (二) 08:34 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

$μ = μ_{0} e x p (β \sqrt{E})$

Where　

$μ_{0}$ is the zero-field mobility
$β$ is the factor of mobility increasing
$E$ is the electric field.

Format

$usemunpfunc
1 μe βe μh βh

Parameter Explanation

μe : electron zero-field mobility $(c m^{2} e V^{- 1} s^{- 1})$
βe : electron beta $(e V^{- 1 / 2})$
μh : hole zero-field mobility $(c m^{2} e V^{- 1} s^{- 1})$
βh : hole beta $(e V^{- 1 / 2})$

@@ 第1行： / 第1行： @@
 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
-<big><big>'''format'''</big></big>
+<math>\mu=\mu_0 exp(\beta\sqrt{E})</math>
+Where
+* <math>\mu_0</math> is the zero-field mobility
+* <math>\beta</math> is the factor of mobility increasing
+* <math>E</math> is the electric field.
+<big><big>'''Format'''</big></big>
   $usemunpfunc
-mue0 betae muh0 betah
+μe βe μh βh
- parameter explanation
+'''<big><big>Parameter Explanation</big></big>'''
-mue0 u8efbc9aelectron mobility at e 0 unit cm 2 ev -1 s -1
+* μe : electron zero-field mobility <math>(cm^{2}eV^{-1}s^{-1})</math>
-betae u8efbc9aelectron beta unit ev -0.5
+* βe : electron beta <math>(eV^{-1/2})</math>
-muh0 u8efbc9ahole mobility at e 0 unit cm 2 ev -1 s -1
+* μh : hole zero-field mobility <math>(cm^{2}eV^{-1}s^{-1})</math>
-betah u8efbc9ahole beta unit ev -0.5
+* βh : hole beta <math>(eV^{-1/2})</math>

「$usemunpfunc」：修訂間差異

於 2017年8月15日 (二) 08:34 的修訂

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