| ... | @@ -62,7 +62,7 @@ $`\vec{j}_{\downarrow}(r) = \sum_{|E_n|<E_c} \textrm{Im}[v_{n,\downarrow}(r)\nab |
... | @@ -62,7 +62,7 @@ $`\vec{j}_{\downarrow}(r) = \sum_{|E_n|<E_c} \textrm{Im}[v_{n,\downarrow}(r)\nab |
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In these formulas $`E_{n}`$ denotes quasi-particle energy and $`E_c`$ is energy cut-off scale. Fermi distribution function $`f_{\beta}(E)=1/(\exp(\beta E)+1)`$ is introduced to model temperature $`T=1/\beta`$ effects.
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In these formulas $`E_{n}`$ denotes quasi-particle energy and $`E_c`$ is energy cut-off scale. Fermi distribution function $`f_{\beta}(E)=1/(\exp(\beta E)+1)`$ is introduced to model temperature $`T=1/\beta`$ effects.
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Densities are accessible for user through structure [wslda_density](https://gitlab.fizyka.pw.edu.pl/gabrielw/wslda/-/tree/public/hpc-engine/wslda_potdens.h):
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Densities are accessible for user through structure [wslda_density](https://gitlab.fizyka.pw.edu.pl/wtools/wslda/-/tree/public/hpc-engine/wslda_potdens.h):
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```c
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```c
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typedef struct
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typedef struct
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{
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{
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| ... | @@ -107,7 +107,7 @@ $`\vec{A}_{\sigma}=\dfrac{\delta\mathcal{E}_{\textrm{edf}}}{\delta \vec{j}_{\sig |
... | @@ -107,7 +107,7 @@ $`\vec{A}_{\sigma}=\dfrac{\delta\mathcal{E}_{\textrm{edf}}}{\delta \vec{j}_{\sig |
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* `delta`:
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* `delta`:
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$`\Delta(r)=-\dfrac{\delta\mathcal{E}_{\textrm{edf}}}{\delta \nu^*}`$ -- paring potential.
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$`\Delta(r)=-\dfrac{\delta\mathcal{E}_{\textrm{edf}}}{\delta \nu^*}`$ -- paring potential.
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Potentials are accessible for user through structure [wslda_potential](https://gitlab.fizyka.pw.edu.pl/gabrielw/wslda/-/tree/public/hpc-engine/wslda_potdens.h):
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Potentials are accessible for user through structure [wslda_potential](https://gitlab.fizyka.pw.edu.pl/wtools/wslda/-/tree/public/hpc-engine/wslda_potdens.h):
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```c
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```c
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typedef struct
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typedef struct
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{
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{
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| ... | | ... | |
