"$usemunpfunc" 修訂間的差異

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<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>
   
−
If <math> \mu_{n,temp} \times E > v_{n,sat}, then {\mu_n} = \frac{1\v_{n,sat}}{E} </math>
 +
If <math> \mu_{n,temp} \times E > v_{n,sat}, then \mu_n = \frac{v_{n,sat}}{E} </math>
−
If <math> \mu_{n,temp} \times E > v_{n,sat}, then {\mu_n} = \frac{1\v_{n,sat}}{E} </math>
 +
If <math> \mu_{p,temp} \times E > v_{p,sat}, then \mu_p = \frac{v_{p,sat}}{E} </math>

於 2018年3月26日 (一) 10:21 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


\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 

\mu_n=\mu_0 exp(\beta\sqrt{E}),  \mu_p=\mu_0 exp(\beta\sqrt{E})
  • 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})


$usemunpfunc
11 μe βe μh βh v_{n,sat} v_{p,sat}


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})
  • v_{n,sat} saturate electron velocity (cm/s)
  • v_{p,sat} saturate hole velocity (cm/s)
 \mu_{n,temp}=\mu_0 exp(\beta\sqrt{E}),  \mu_{p,temp}=\mu_0 exp(\beta\sqrt{E}) 

 If  \mu_{n,temp} \times E > v_{n,sat}, then \mu_n = \frac{v_{n,sat}}{E} 
 If  \mu_{p,temp} \times E > v_{p,sat}, then \mu_p = \frac{v_{p,sat}}{E}
取自 "http://yrwu-wk.ee.ntu.edu.tw/mediawiki/index.php?title=$usemunpfunc&oldid=838"