"*.vg *-pl.info" 修訂間的差異
出自 DDCC TCAD TOOL Manual
(未顯示同一使用者於中間所作的 19 次修訂) | |||
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end |
end |
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− | For n=1,C_e_N |
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− | for m=1,V_HH_M |
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− | for Ei=0, Emax |
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− | end |
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+ | Rsp=0.0 |
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− | end |
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+ | <math> const = \frac{1}{3} \frac{e_{0}^{2} * n_{r}}{2\pi\epsilon_{0}*m_{0}*c^3\hbar^2} * Ep </math> |
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+ | <math> N_{2D} = \frac{ m_r^* }{\pi\hbar^2} </math> |
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+ | <math>For~~ n=1,~C_{e,n} </math> |
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+ | <math>for~~ m=1,V_{HH,m} </math> |
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+ | <math>for~~ E_{\hbar\omega}=0,~~ Emax </math> |
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+ | <math>for~~ Ek = Ei - 5\sigma~~ ,~~ Ei+5\sigma </math> |
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+ | <math> If Ek > E_{n,e}-E_{hh,m} =E_{g,eff} then </math> |
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+ | <math> Ee = E_{e,n} +(Ek-E_{g,eff}) * \frac{m_r^{*}}{m_{e}^{*}} </math> |
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+ | <math> Ehh = E_{hh,m}-(Ek-E_{g,eff}) * \frac{m_r^{*}}{m_{hh}^{*}} </math> |
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+ | <math>end </math> |
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+ | <math>end</math> |
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+ | The PL of e to LH can be calculated by |
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+ | Rsp=0.0 |
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+ | <math>For~~ n=1,~C_{e,n} </math> |
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+ | <math>for~~ m=1,V_{LH,m} </math> |
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+ | <math>for~~ E_{\hbar\omega}=0,~~ Emax </math> |
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+ | <math>for~~ Ek = Ei - 5\sigma~~ ,~~ Ei+5\sigma </math> |
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+ | <math> If Ek > E_{g,eff} = E_{n,e}-E_{lh,m} </math> |
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+ | <math> Ee = E_{e,n} +(Ek-E_{g,eff}) * \frac{m_r^{*}}{m_{e}^{*}} </math> |
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+ | <math> Elh = E_{lh,m}-(Ek-E_{g,eff}) * \frac{m_r^{*}}{m_{lh}^{*}} </math> |
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+ | <math> fe = \frac{1}{1+exp(\frac{Ee-Efn}{k_BT})} </math> |
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+ | <math> fh = \frac{1}{1+exp(\frac{Efp-Elh}{k_BT})} </math> |
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+ | <math> Rsp(Ei) = Rsp(Ei) + const*dE * Ei * |\langle\phi_{e,n} |\phi_{lh,m} \rangle |^2 * fe * fh* \frac{1}{\sqrt{2\pi} \sigma} exp( -\frac{(Ek-Ei)^2}{2*\sigma^2}) * N_{2D} </math> |
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+ | <math>end ~~if</math> |
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+ | <math>end</math> |
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+ | <math>end </math> |
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+ | <math>end </math> |
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+ | <math>end</math> |
於 2025年1月28日 (二) 16:27 的最新修訂
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![]()
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The PL of e to LH can be calculated by
Rsp=0.0![]()
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