"$usemunpfunc" 修訂間的差異

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

於 2018年3月26日 (一) 10:14 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


\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 \mu_{n,sat} \mu_{p,sat}


Parameter Explanation type:

  • 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})
  • \mu_{n,sat} saturate electron mobility
  • \mu_{p,sat} saturate hole mobility
 \mu_{n,temp}=\mu_0 exp(\beta\sqrt{E}),  \mu_{p,temp}=\mu_0 exp(\beta\sqrt{E}) 
  \frac{1}{\mu_n} = \frac{1}{\mu_{n,temp}} + \frac{1}{\mu_{n,sat}}
取自 "http://yrwu-wk.ee.ntu.edu.tw/mediawiki/index.php?title=$usemunpfunc&oldid=832"