檢視 .vg -pl.info 的原始碼

 C_e_N, V_HH_M, V_LH_L, nr , Epp
 For n=1,C_e_N
   for m=1,V_HH_M
     <math> C_{n},~ V_{hh,m}, ~|\langle \phi_{e,n},\phi_{hh,m}\rangle |^{2},~ E_{n,e}-E_{hh,m},~ E_{e,n},~E_{fn},~E_{fp},~m_{e},~m_hh, N_{2D,DOS,r} </math>
   end 
 end
 For n=1,C_e_N
   for m=1,V_LH_L
     <math> C_{n},~ V_{lh,m}, ~|\langle \phi_{e,n},\phi_{lh,m}\rangle |^{2},~ E_{n,e}-E_{lh,m},~ E_{e,n},~E_{fn},~E_{fp},~m_{e},~m_lh, N_{2D,DOS,r} </math>
   end 
 end

The PL of e to HH can be calculated by 
 Rsp=0.0 
 For n=1,C_e_N
   for m=1,V_HH_M
      for E_{\hbar\omega}=0, Emax
          for Ek = <math>Ei - 5\sigma , Ei+5\sigma </math>  
             <math> If Ek >  E_{n,e}-E_{hh,m} =E_{g,eff} then  </math>    
             <math> Ee =  E_{e,n} +(Ek-E_{g,eff}) * \frac{m_r^{*}}{m_{e}^{*}} </math> 
             <math> Ehh = E_{hh,m}-(Ek-E_{g,eff}) * \frac{m_r^{*}}{m_{hh}^{*}} </math>         
             <math> fe = \frac{1}{1+exp(\frac{Ek-Efn}{k_BT})} </math>
             <math> fh = \frac{1}{1+exp(\frac{Efp-Ek}{k_BT})} </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>
          end
      end 
   end 
 end

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             
             <math> fe = \frac{1}{1+exp(\frac{Ek-Efn}{k_BT})} </math>
             <math> fh = \frac{1}{1+exp(\frac{Efp-Ek}{k_BT})} </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>
          end
      end 
   end 
 end