mirror of https://github.com/phonopy/phono3py.git
Update document
This commit is contained in:
parent
2d89ae237e
commit
cf1a4279de
|
@ -595,6 +595,8 @@ where $N$ is the number of grid points on the sampling mesh.
|
|||
$\Phi_{\lambda \lambda' \lambda''} \equiv 0$ unless
|
||||
$\mathbf{q} + \mathbf{q}' + \mathbf{q}'' = \mathbf{G}$.
|
||||
|
||||
See also references {cite}`Togo-PRB-2015,Mizokami-PRB-2018`.
|
||||
|
||||
This option works only when `--read-gamma` and `--br` options are activated
|
||||
where the averaged phonon-phonon interaction that is read from
|
||||
`kappa-mxxx(-sx-sdx).hdf5` file is used if it exists in the file. Therefore the
|
||||
|
@ -623,7 +625,8 @@ constant value and $|\Phi_{\lambda \lambda'
|
|||
{ref}`--ave-pp <ave_pp_option>` for thermal conductivity calculation. This
|
||||
option works only when `--br` options are activated. Therefore third-order force
|
||||
constants are not necessary to input. The physical unit of the value is
|
||||
$\text{eV}^2$.
|
||||
$\text{eV}^2$. See also references {cite}`Togo-PRB-2015,Mizokami-PRB-2018`.
|
||||
|
||||
|
||||
```bash
|
||||
% phono3py --dim="3 3 2" -v --mesh="32 32 20" -c POSCAR-unitcell --br --const-ave-pp=1e-10
|
||||
|
@ -814,7 +817,7 @@ $$
|
|||
|
||||
respectively. In the above formulae, angular frequency $\omega$ is used, but in
|
||||
the calculation results, ordinal frequency $\nu$ is used. Be careful about
|
||||
$2\pi$ treatment. See also {cite}`Togo-PRB-2015,Togo-JPCM-2022`.
|
||||
$2\pi$ treatment. See also references {cite}`Togo-PRB-2015,Togo-JPCM-2022`.
|
||||
|
||||
(ise_option)=
|
||||
|
||||
|
@ -878,7 +881,7 @@ $$
|
|||
\int_0^\infty \frac{d\omega}{2\pi} A_\lambda(\omega) = 1.
|
||||
$$
|
||||
|
||||
See also {cite}`Togo-JPCM-2022`.
|
||||
See also reference {cite}`Togo-JPCM-2022`.
|
||||
|
||||
### `--spf` (`SPECTRAL_FUNCTION = .TRUE.`)
|
||||
|
||||
|
@ -934,7 +937,7 @@ $$
|
|||
\end{align}
|
||||
$$
|
||||
|
||||
(See also {cite}`Togo-PRB-2015,Togo-JPCM-2022`.)
|
||||
(See also references {cite}`Togo-PRB-2015,Togo-JPCM-2022`.)
|
||||
|
||||
```bash
|
||||
% phono3py --fc2 --dim="2 2 2" --pa="F" -c POSCAR-unitcell --mesh="16 16 16" --jdos --ga="0 0 0 8 8 8"
|
||||
|
@ -960,7 +963,7 @@ $$
|
|||
\end{align}
|
||||
$$
|
||||
|
||||
(See also {cite}`Togo-PRB-2015,Mizokami-PRB-2018,Togo-JPCM-2022`.)
|
||||
(See also references {cite}`Togo-PRB-2015,Mizokami-PRB-2018,Togo-JPCM-2022`.)
|
||||
|
||||
```bash
|
||||
% phono3py --fc2 --dim="2 2 2" --pa="F" -c POSCAR-unitcell --mesh="16 16 16" --jdos --ga="0 0 0 8 8 8" --ts=300
|
||||
|
|
|
@ -1,7 +1,8 @@
|
|||
(command_cutoff_pair)=
|
||||
# Force constants calculation with cutoff pair-distance
|
||||
|
||||
Here the detail of the command option {ref}`--cutoff_pair <cutoff_pair_option>` is explained.
|
||||
Here the detail of the command option {ref}`--cutoff_pair <cutoff_pair_option>`
|
||||
is explained. See also reference {cite}`Mizokami-PRB-2018`.
|
||||
|
||||
```{contents}
|
||||
:depth: 2
|
||||
|
@ -427,3 +428,8 @@ number_of_pairs_in_cutoff: 1248
|
|||
300.0 235.642 235.642 219.348 0.000 -0.000 -0.000
|
||||
300.0 235.728 235.728 219.102 0.000 -0.000 -0.000
|
||||
```
|
||||
|
||||
## References
|
||||
```{bibliography}
|
||||
:filter: docname in docnames
|
||||
```
|
||||
|
|
Loading…
Reference in New Issue