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nnp:optics:internal_quantum_efficiency [2017/02/02 17:32]
stefan.birner [Physics Model]
nnp:optics:internal_quantum_efficiency [2017/02/03 10:19] (current)
stefan.birner [Recombination]
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 ====== Emission: Internal Quantum Efficiency ====== ====== Emission: Internal Quantum Efficiency ======
  
-In this tutorial we demonstrate how to calculate the internal quantum efficiency of a multi-quantum well structure as the function of the applied forward bias.+In this tutorial we demonstrate how to calculate the internal quantum efficiency of a multi-quantum well structure as function of the applied forward bias.
  
 ==== Physics Model ====  ==== Physics Model ==== 
  
 **nextnano++** is capable of simulating recombination processes such as //​Shockley-Read-Hall (SRH)//, //Auger// and //​radiative//​ recombination. **nextnano++** is capable of simulating recombination processes such as //​Shockley-Read-Hall (SRH)//, //Auger// and //​radiative//​ recombination.
-Only the radiative //​(direct)//​ recombination process ​generates photons ​(spontaneous emission). +Only the radiative //​(direct)//​ recombination process (spontaneous emission) ​generates photons
-If it is summed up over the full device, it equals the total number of photons emitted from the device per second, the photocurrent:​ $I_{\rm photon}$.+If radiative recombination $R_{\rm sp}(x)$ ​is summed up over the full device, it equals the total number of photons emitted from the device per second, the photocurrent:​ $I_{\rm photon}$.
  
 ;#; ;#;
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-If the injected charge carrier current is $I_{charge}$, ​than the internal quantum efficiency is+If the injected charge carrier current is $I_{\rm charge}$, ​then the internal quantum efficiency ​$\eta_{\rm qe}$ is
 ;#; ;#;
-$$\eta_{qe} = \frac{I_{photon}}{I_{charge}}$$ ​+$$\eta_{\rm qe} = \frac{I_{\rm photon}}{I_{\rm charge}}$$ ​
  
 ;#; ;#;
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 </​Code>​ </​Code>​
  
-The internal quantum efficiency is automatically ​calculated when the radiative recombination is switched on+The internal quantum efficiency is calculated ​automatically ​when the radiative recombination is switched on
 <​Code>​ <​Code>​
      ​radiative ​     = yes       # radiative recombination (direct recombination)      ​radiative ​     = yes       # radiative recombination (direct recombination)
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 ==== Bandstructure ==== ==== Bandstructure ====
-The band structure of the **MQW** structure can be seen of figure {{ref>​bandstructure}} without bias voltage.+The band structure of the **MQW** structure can be seen in figure {{ref>​bandstructure}} without bias voltage.
 <figure bandstructure>​ <figure bandstructure>​
 ;#; ;#;
-<​dataplot center linepoints xrange=-100.0:​180.0 yrange=-3.0:​2.0 xlabel="​x(nm)" ylabel="​E(eV)" ylegends="​Gamma LH HH SO Fermi_{electron} Fermi_{hole}"​ legendpos="​right bottom"​ 600x400>+<​dataplot center linepoints xrange=-100.0:​180.0 yrange=-3.0:​2.0 xlabel="​Position ​(nm)" ylabel="​Energy ​(eV)" ylegends="​Gamma LH HH SO Fermi_{electron} Fermi_{hole}"​ legendpos="​right bottom"​ 600x400>
 -121 -0 -0 -0 -0 0 0 -121 -0 -0 -0 -0 0 0
 -120.001 -0 -0 -0 -0 0 0 -120.001 -0 -0 -0 -0 0 0
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 </​dataplot>​ </​dataplot>​
 ;#; ;#;
-<​caption>​Bandstructure with zero bias. Two Quantum ​wells with alloy structures //In(0.7)Ga(0.3)As//, and well barriers ​ //In(0.53)Ga(0.47)As// </​caption>​+<​caption>​Band structure at zero bias. The two quantum ​wells consist of ${\rm In}_{0.7}{\rm Ga}_{0.3}{\rm As}$ and are surrounded by ${\rm In}_{0.53}{\rm Ga}_{0.47}{\rm As}$ barriers.</​caption>​
 </​figure>​ </​figure>​
  
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 <figure recombination>​ <figure recombination>​
 ;#; ;#;
-<​dataplot center linepoints xrange=-50.0:​150.0 xlabel="​x(nm)" ylabel="​I(1/​cm^3/​s)"​ ylegends="​total SRH Auger radiative"​ legendpos="​right top" 600x400>+<​dataplot center linepoints xrange=-50.0:​150.0 xlabel="​Position ​(nm)" ylabel="​(1/​cm^3/​s)"​ ylegends="​total SRH Auger radiative"​ legendpos="​right top" 600x400>
 -121 0 0 0 0 -121 0 0 0 0
 -120 1249.9986884573 1249.9986884573 0 0 -120 1249.9986884573 1249.9986884573 0 0
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 </​dataplot>​ </​dataplot>​
 ;#; ;#;
-<​caption>​Comparison of different recombination processes</​caption>​+<​caption>​Comparison of different recombination processes. The applied bias is 1 V.</​caption>​
 </​figure>  ​ </​figure>  ​
  
  
-==== UI Characteristics====+==== Current-Voltage ​Characteristics====
  
-The $I-U$ characteristics of the device is plotted in figure {{ref>​IUchar}}, where additionally ​the full photo-current ​is plotted+The $I-V$ characteristics of the device is plotted in figure {{ref>​IUchar}}
 +This figure also includes ​the full photo current. ​
  
 <figure IUchar> <figure IUchar>
 ;#; ;#;
  
-<​dataplot center linepoints xlabel="​U_{bias}(V)" ylabel="​I(A/​cm^2)"​ ylegends="​I_{Right} I_{Left} I_{photo}"​ legendpos="​left top" 600x400>+<​dataplot center linepoints xlabel="​Voltage ​(V)" ylabel="​Current density ​(A/​cm^2)"​ ylegends="​I_{right} I_{left} I_{photo}"​ legendpos="​left top" 600x400>
 0 0.0048007999 -0.004800798 8.5567076e-05 ​ 0 0.0048007999 -0.004800798 8.5567076e-05 ​
 0.1 7.8561578 -7.8561504 8.9688789e-05 ​ 0.1 7.8561578 -7.8561504 8.9688789e-05 ​
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 </​dataplot>​ </​dataplot>​
 ;#; ;#;
-<​caption>​$I-Ucharacteristic ​of the device ​with additional ​photo-current. The device ​had just two contacts ​which means the charge carrier ​currents on the left and the right contacts ​are equal in absolute value.</​caption>​+<​caption>​$I-Vcharacteristics ​of the device ​and photo current. The device ​has two contacts ​and the charge carrier ​current densities at the left and at the right contact ​are equal in absolute value.</​caption>​
 </​figure>​ </​figure>​
  
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 ;#; ;#;
  
-<​dataplot center linepoints yrange=-0.005:​0.8 xlabel="​U_{bias}(V)" ylabel="​IQE(-)" ylegends=""​ 600x400>+<​dataplot center linepoints yrange=-0.005:​0.8 xlabel="​Voltage ​(V)" ylabel="​IQE"​ ylegends=""​ 600x400>
 0 0.017823508 ​ 0 0.017823508 ​
 0.1 1.1416374e-05 ​ 0.1 1.1416374e-05 ​
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 </​dataplot>​ </​dataplot>​
 ;#; ;#;
-<​caption>​Internal quantum efficiency ​in the function of the forward bias voltage</​caption>​+<​caption>​Internal quantum efficiency ​as a function of the forward bias voltage</​caption>​
 </​figure>​ </​figure>​
  
nnp/optics/internal_quantum_efficiency.1486056752.txt.gz · Last modified: 2017/02/02 17:32 (external edit)