"$ifapplyEgofT" 修訂間的差異
| (未顯示由 2 位使用者於中間所作的 6 次修訂) | |||
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| − | Since the DDCC has the capability of solving the Poisson, drift-diffusion, and thermal solver self-consistently. It will need to consider the possibility of bandgap narrowing with temperature. Therefore, we can apply the temperature |
+ | Since the DDCC has the capability of solving the Poisson, drift-diffusion, and thermal solver self-consistently. It will need to consider the possibility of bandgap narrowing with temperature. Therefore, we can apply the temperature-dependent coefficients for the material's bandgap. Usually, the temperature-dependent bandgap can be expressed as: <br> |
| − | <math> Eg(T) = Eg(0) - \frac{\gamma T^{2} }{ T + \beta} </math> |
+ | <math> Eg(T) = Eg(0) - \frac{\gamma \times T^{2} }{ T + \beta} </math> |
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| + | In the program, we don't set Eg(0), instead, we set Eg(300) |
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| + | <math> Eg(T) = Eg(300) + \frac{\gamma \times 300^{2} }{ 300 + \beta} - \frac{\gamma \times T^{2} }{ T + \beta} </math> |
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$ifapplyEgofT |
$ifapplyEgofT |
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| − | Eg( |
+ | <math>Eg(300)_{1} </math> <math> \gamma </math> <math> \beta </math> |
| − | Eg( |
+ | <math>Eg(300)_{2} </math> <math> \gamma </math> <math> \beta </math> |
| − | Eg( |
+ | <math>Eg(300)_{3} </math> <math> \gamma </math> <math> \beta </math> |
| − | Eg( |
+ | <math>Eg(300)_{4} </math> <math> \gamma </math> <math> \beta </math> |
... |
... |
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... |
... |
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If some material's coefficient cannot be found, please make <math> \gamma = 0 </math>. So the program will keep the bandgap of this region as constant. <br> |
If some material's coefficient cannot be found, please make <math> \gamma = 0 </math>. So the program will keep the bandgap of this region as constant. <br> |
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Note that <br> |
Note that <br> |
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| − | Eg( |
+ | Eg(300) is the Eg at 300K. With this modified equation, we can make the Eg is always the same as the original Eg at 300K |
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| + | <br><br> |
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| + | For advanced users who use libmodpar.f90. This function may have a problem if the bandgap is changed in libmodpar.f90 |
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| + | <big>'''The $ifapplyEgofT setting for 1D-DDCC in GUI interface '''</big> <br> |
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| + | The parameters are modified in '''Step 4'''.<br> |
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| + | [[檔案:1d_$ifapplyEgofT_fig1.jpg|1300px]]<br> |
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| + | <br>'''<big><big>The $ifapplyEgofT setting for 2D-DDCC in GUI interface</big></big>''' <br> |
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| + | Press '''Thermal''', check the box and set the fields as needed!<br> |
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| + | [[檔案:2D_ifapplyEgofT_fig1.jpg|1200px]]<br><br> |
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| + | The related commands are: [[$ifapplytauofT]], [[$ifapplymuofT]], [[$ifapplyEgofT]], [[$ifTversusJ]] |
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於 2024年11月22日 (五) 18:25 的最新修訂
Since the DDCC has the capability of solving the Poisson, drift-diffusion, and thermal solver self-consistently. It will need to consider the possibility of bandgap narrowing with temperature. Therefore, we can apply the temperature-dependent coefficients for the material's bandgap. Usually, the temperature-dependent bandgap can be expressed as:
In the program, we don't set Eg(0), instead, we set Eg(300)
Therefore, to enable the temperature-dependent Eg in the simulation, we need to add
.
$ifapplyEgofT
If some material's coefficient cannot be found, please make 
. So the program will keep the bandgap of this region as constant.
Note that
Eg(300) is the Eg at 300K. With this modified equation, we can make the Eg is always the same as the original Eg at 300K
For advanced users who use libmodpar.f90. This function may have a problem if the bandgap is changed in libmodpar.f90
The $ifapplyEgofT setting for 1D-DDCC in GUI interface
The parameters are modified in Step 4.
The $ifapplyEgofT setting for 2D-DDCC in GUI interface
Press Thermal, check the box and set the fields as needed!
The related commands are: $ifapplytauofT, $ifapplymuofT, $ifapplyEgofT, $ifTversusJ
