「$2Dexcitonpar」：修訂間差異
無編輯摘要 |
無編輯摘要 |
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| （未顯示同一使用者於中間所作的 3 次修訂） | |||
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$2Dexcitonpar is the command to solve the exciton diffusion equations. Actually the exciton solver is an external function | $2Dexcitonpar is the command to solve the exciton diffusion equations. Actually, the exciton solver is an external function that is currently under development. Therefore, there is no clear definition of excitation parameters.<br> | ||
The related commands are [[$2Dexcitonmode]] | |||
[[$call2Dexciton]]<br> | |||
The user can define their own definition of these parameters. The format is | |||
$2Dexcitonpar | $2Dexcitonpar | ||
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excitonpar(5,n) -> K_SE -> exciton - electron quench | excitonpar(5,n) -> K_SE -> exciton - electron quench | ||
excitonpar(6,n) -> K_SH -> exciton - hole quench | excitonpar(6,n) -> K_SH -> exciton - hole quench | ||
For example: | |||
$2Dexcitonmode | |||
1 1 | |||
$2Dexcitonpar | |||
6 | |||
1.0e-7 1.0e7 3.0e7 1.0e-10 1.0e-5 2.0e-5 | |||
1.0e-7 1.0e7 3.0e7 1.0e-10 1.0e-5 2.0e-5 | |||
1.0e-7 1.0e7 3.0e7 1.0e-10 1.0e-5 2.0e-5 | |||
.... N region need to have N layers | |||
The summary of each loss will be outputted to the sum.json file | |||
The user will use these parameters in [[subroutine exciton2Dquench( )]]. <br> | The user will use these parameters in [[subroutine exciton2Dquench( )]]. <br> | ||
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Related commands: <br> | Related commands: <br> | ||
[[$call2Dexciton]]<br> | [[$call2Dexciton]], [[$2Dexcitonmode]]<br> | ||
於 2025年11月4日 (二) 09:06 的最新修訂
$2Dexcitonpar is the command to solve the exciton diffusion equations. Actually, the exciton solver is an external function that is currently under development. Therefore, there is no clear definition of excitation parameters.
The related commands are $2Dexcitonmode
$call2Dexciton
The user can define their own definition of these parameters. The format is
$2Dexcitonpar N_column excitonpar(1,1) excitonpar(2,1) excitonpar(3,1) excitonpar(4,1) excitonpar(5,1) ... excitonpar(N_column,1) excitonpar(1,2) excitonpar(2,2) excitonpar(3,2) excitonpar(4,2) excitonpar(5,2) ... excitonpar(N_column,2) excitonpar(1,3) excitonpar(2,3) excitonpar(3,3) excitonpar(4,3) excitonpar(5,3) ... excitonpar(N_column,3) excitonpar(1,4) excitonpar(2,4) excitonpar(3,4) excitonpar(4,4) excitonpar(5,4) ... excitonpar(N_column,4) ... ... ... ... excitonpar(1,n) excitonpar(2,n) excitonpar(3,n) excitonpar(4,n) excitonpar(5,n) ... excitonpar(N_column,n)
At 10/01/2024: par 1-6 are defined as
excitonpar(1,n) -> D_ex -> diffusion coefficient excitonpar(2,n) -> Kr -> exciton radiative recombination excitonpar(3,n) -> Knr -> exciton non-radiative recombination excitonpar(4,n) -> -> exciton exciton quench excitonpar(5,n) -> K_SE -> exciton - electron quench excitonpar(6,n) -> K_SH -> exciton - hole quench
For example:
$2Dexcitonmode 1 1
$2Dexcitonpar 6 1.0e-7 1.0e7 3.0e7 1.0e-10 1.0e-5 2.0e-5 1.0e-7 1.0e7 3.0e7 1.0e-10 1.0e-5 2.0e-5 1.0e-7 1.0e7 3.0e7 1.0e-10 1.0e-5 2.0e-5 .... N region need to have N layers
The summary of each loss will be outputted to the sum.json file
The user will use these parameters in subroutine exciton2Dquench( ).
The $2Dexcitonpar setting in GUI interface is here
After setting up the general structure, press OLED Setting, check the box, and fill in the fields for Dr, Kr, Knr, and Gamma as needed!
Related commands:
$call2Dexciton, $2Dexcitonmode