"$usemunpfunc" 修訂間的差異

於 2017年8月15日 (二) 16:34 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

$\mu=\mu_0 exp(\beta\sqrt{E})$

Where　

$\mu_0$ is the zero-field mobility
$\beta$ 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 $(cm^{2}eV^{-1}s^{-1})$
βe : electron beta $(eV^{-1/2})$
μh : hole zero-field mobility $(cm^{2}eV^{-1}s^{-1})$
βh : hole beta $(eV^{-1/2})$

@@ 行 1： / 行 1： @@
 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" 修訂間的差異

於 2017年8月15日 (二) 16:34 的修訂

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