「$usemunpfunc」：修訂間差異

於 2018年3月26日 (一) 02:14 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

 $μ_{n} = μ_{0} e x p (β \sqrt{E})$ ,   $μ_{p} = μ_{0} e x p (β \sqrt{E})$

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. $(e V^{- 1 / 2})$

$usemunpfunc
11 μe βe μh βh  $μ_{n, s a t}$   $μ_{p, s a t}$

Parameter Explanation type:

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. $(e V^{- 1 / 2})$
$μ_{n, s a t}$ saturate electron mobility
$μ_{p, s a t}$ saturate hole mobility

  $μ_{n, t e m p} = μ_{0} e x p (β \sqrt{E})$ ,   $μ_{p, t e m p} = μ_{0} e x p (β \sqrt{E})$  
  $\frac{1}{μ_{n}} = \frac{1}{μ_{n, t e m p}} + \frac{1}{μ_{n, s a t}}$

@@ 第17行： / 第17行： @@
   $usemunpfunc
 μe βe μh βh
 '''<big><big>Parameter Explanation</big></big>'''
+ <math>\mu_n=\mu_0 exp(\beta\sqrt{E})</math>,  <math>\mu_p=\mu_0 exp(\beta\sqrt{E})</math>
 * μe : electron zero-field mobility. <math>(cm^{2}eV^{-1}s^{-1})</math>
 * βe : electron beta. <math>(eV^{-1/2})</math>
 * μh : hole zero-field mobility. <math>(cm^{2}eV^{-1}s^{-1})</math>
 * βh : hole beta. <math>(eV^{-1/2})</math>
+ $usemunpfunc
+μe βe μh βh <math>\mu_{n,sat}</math> <math>\mu_{p,sat}</math>
+'''<big><big>Parameter Explanation</big></big>'''
+type: <br>
+* μe : electron zero-field mobility. <math>(cm^{2}eV^{-1}s^{-1})</math>
+* βe : electron beta. <math>(eV^{-1/2})</math>
+* μh : hole zero-field mobility. <math>(cm^{2}eV^{-1}s^{-1})</math>
+* βh : hole beta. <math>(eV^{-1/2})</math>
+* <math>\mu_{n,sat}</math>  saturate electron mobility
+* <math>\mu_{p,sat}</math>  saturate hole mobility
+  <math>\mu_{n,temp}=\mu_0 exp(\beta\sqrt{E})</math>,  <math>\mu_{p,temp}=\mu_0 exp(\beta\sqrt{E})</math>
+  <math> \frac{1}{\mu_n} = \frac{1}{\mu_{n,temp}} + \frac{1}{\mu_{n,sat}} </math>

「$usemunpfunc」：修訂間差異

於 2018年3月26日 (一) 02:14 的修訂

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