"*.vg *-pl.info" 修訂間的差異
出自 DDCC TCAD TOOL Manual
行 13: | 行 13: | ||
The PL of e to HH can be calculated by |
The PL of e to HH can be calculated by |
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Rsp=0.0 |
Rsp=0.0 |
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− | For n=1,C_e_N |
+ | <math>For n=1,C_e_N </math> |
− | for m=1,V_HH_M |
+ | <math>for m=1,V_HH_M </math> |
<math>for E_{\hbar\omega}=0, Emax </math> |
<math>for E_{\hbar\omega}=0, Emax </math> |
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<math>for Ek = Ei - 5\sigma , Ei+5\sigma </math> |
<math>for Ek = Ei - 5\sigma , Ei+5\sigma </math> |
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行 23: | 行 23: | ||
<math> fh = \frac{1}{1+exp(\frac{Efp-Ehh}{k_BT})} </math> |
<math> fh = \frac{1}{1+exp(\frac{Efp-Ehh}{k_BT})} </math> |
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<math> Rsp(Ei) = Rsp(Ei) + dE * Ei * |\langle\phi_{e,n} |\phi_{hh,m} \rangle |^2 * fe * fh* \frac{1}{\sqrt{2\pi} \sigma} exp( -\frac{(Ek-Ei)^2}{2*\sigma^2}) </math> |
<math> Rsp(Ei) = Rsp(Ei) + dE * Ei * |\langle\phi_{e,n} |\phi_{hh,m} \rangle |^2 * fe * fh* \frac{1}{\sqrt{2\pi} \sigma} exp( -\frac{(Ek-Ei)^2}{2*\sigma^2}) </math> |
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− | end |
+ | <math>end</math> |
− | end |
+ | <math>end </math> |
− | end |
+ | <math>end </math> |
− | end |
+ | <math>end</math> |
The PL of e to LH can be calculated by |
The PL of e to LH can be calculated by |
於 2025年1月28日 (二) 16:04 的修訂
C_e_N, V_HH_M, V_LH_L, nr , Epp For n=1,C_e_N for m=1,V_HH_Mend end For n=1,C_e_N for m=1,V_LH_L
end end
The PL of e to HH can be calculated by
Rsp=0.0 解析失敗 (PNG 轉換失敗;請檢查是否正確安裝了 latex 與 dvipng (或 dvips + gs + convert)): For n=1,C_e_N![]()
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The PL of e to LH can be calculated by
Rsp=0.0 For n=1,C_e_N for m=1,V_LH_: for Ei=0, Emax for Ek = Ei - 5\sigma , Ei+5\sigma![]()
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end end end end