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# Static and time-dependent codes
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There are two main branches of codes:
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* Static codes `st-wslda-?d` for solving self-consistently static DFT equations
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* Static codes `st-wslda-?d` for solving self-consistently static DFT equations.
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* Time-dependent codes `td-wslda-?d` for solving time dependent DFT equations. The `td-wslda-?d` codes require starting point for the time evolution (i.e $`\psi(\vec{r},t=0)`$) which is typically generated by the static codes.
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In codes names `?` stand for dimensionality, as described below.
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... | ... | @@ -14,7 +14,7 @@ In 2D codes the wave-functions are assumed to be: |
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%5Cfrac%7B1%7D%7B%5Csqrt%7BL_z%7D%7De%5E%7Bik_z%20z%7D%0A)
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where
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%20%5Cfrac%7B2%5Cpi%7D%7BL_z%7D%0A)
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For `NZ=1` the code solves 2D problem (there is only one mode in z-directions, which reduces to 1). Note however, that 2D problem requires different prescription for coupling constant regularization than the one implemented in w-SLDA toolkit.
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For `NZ=1` the code solves 2D problem (there is only one mode in z-directions, which reduces to 1). Note however, that 2D problem requires different prescription for coupling constant regularization than the one implemented in W-SLDA toolkit.
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## 1D codes: `xx-wslda-1d`
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... | ... | @@ -23,4 +23,4 @@ In 1D codes the wave-functions are assumed to be: |
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where
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%20%5Cfrac%7B2%5Cpi%7D%7BL_y%7D%0A)
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%20%5Cfrac%7B2%5Cpi%7D%7BL_z%7D%0A)
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For `NY=1` and `NZ=1` the code solves 1D problem . Note however, that 1D problem requires different prescription for coupling constant regularization than the one implemented in w-SLDA toolkit. |
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\ No newline at end of file |
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For `NY=1` and `NZ=1` the code solves 1D problem . Note however, that 1D problem requires different prescription for coupling constant regularization than the one implemented in W-SLDA toolkit. |
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\ No newline at end of file |