"$negfintervalleyopticalphonon" 修訂間的差異
出自 DDCC TCAD TOOL Manual
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(未顯示同一使用者於中間所作的 2 次修訂) | |||
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<math>W_{op}^{ab}(k)=\frac{\pi D_{op}^{2}}{\rho\omega_{0}}[n(\omega_{0})]I_{if}N_{1D}(E_{k}+\hbar\omega_{0})</math><br> |
<math>W_{op}^{ab}(k)=\frac{\pi D_{op}^{2}}{\rho\omega_{0}}[n(\omega_{0})]I_{if}N_{1D}(E_{k}+\hbar\omega_{0})</math><br> |
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<math>W_{op}^{em}(k)=\frac{\pi D_{op}^{2}}{\rho\omega_{0}}[n(\omega_{0})+1]I_{if}N_{1D}(E_{k}-\hbar\omega_{0})</math><br> |
<math>W_{op}^{em}(k)=\frac{\pi D_{op}^{2}}{\rho\omega_{0}}[n(\omega_{0})+1]I_{if}N_{1D}(E_{k}-\hbar\omega_{0})</math><br> |
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⚫ | |||
+ | |||
$negfintervalleyopticalphonon |
$negfintervalleyopticalphonon |
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<math>\rho</math> <math>\epsilon_{\infty}</math> <math>\epsilon_{s}</math> |
<math>\rho</math> <math>\epsilon_{\infty}</math> <math>\epsilon_{s}</math> |
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行 9: | 行 9: | ||
<math>D_{op2}</math> <math>\omega_{02}</math><br> |
<math>D_{op2}</math> <math>\omega_{02}</math><br> |
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⚫ | |||
$negfintervalleyopticalphonon |
$negfintervalleyopticalphonon |
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2329.0 0.0 11.7 |
2329.0 0.0 11.7 |
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1.760e-8 9.4476e13 |
1.760e-8 9.4476e13 |
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3.328e-9 8.9905e13 |
3.328e-9 8.9905e13 |
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− | # rho epsilon_inf epsilon_s |
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+ | |||
− | # D0 w0 |
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− | # D02 w02 |
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related commands: |
related commands: |
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− | [[$negfifscattering]] |
+ | [[$ifsolvenegf]], [[$negfifscattering]] |
於 2018年7月30日 (一) 09:28 的最新修訂
If you use the command $negfifscattering and the second term is 2, then use the command $negfintervalleyopticalphonon to setup the related parameters of intervalley optical phonon scattering(the g-type and f-type) of Si.
The equation of nonpolar optical phonon scattering(deformation potential scattering):
$negfintervalleyopticalphonon
Example:
$negfintervalleyopticalphonon 2329.0 0.0 11.7 1.760e-8 9.4476e13 3.328e-9 8.9905e13
related commands:
$ifsolvenegf, $negfifscattering