phono3py/doc/_static/procedure.dot

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digraph phonopy {
graph [bgcolor=transparent];
"Phono3py (force-sets)" [shape = box, style = filled];
"Phono3py (FC)" [shape = box, style = filled];
"Phono3py (LTC)" [shape = box, style = filled];
"Force calc." [shape = octagon];
"Force-constants calc." [shape = octagon];
subgraph ph3force {
"Unit cell" -> "Phono3py (force-sets)";
"Supercell matrix" -> "Phono3py (force-sets)";
"Phono3py (force-sets)" -> "Supercell";
"Phono3py (force-sets)" -> "Displacement dataset";
"Supercell" -> "Force calc.";
"Displacement dataset" -> "Force calc.";
"Force calc." -> "Supercell-force sets";
}
subgraph ph3fc {
"Unit cell" -> "Phono3py (FC)";
"Supercell matrix" -> "Phono3py (FC)";
"Displacement dataset" -> "Phono3py (FC)";
"Supercell-force sets" -> "Phono3py (FC)";
"Phono3py (FC)" -> "Force-constants calc.";
"Force-constants calc." -> "Force constants (fc2, fc3)";
}
subgraph ph3ltc {
"Unit cell" -> "Phono3py (LTC)";
"Supercell matrix" -> "Phono3py (LTC)";
"Primitive cell matrix\n(optional)" -> "Phono3py (LTC)";
"Non-analytical term\ncorrection parameters\n(optional)" -> "Phono3py (LTC)";
"Force constants (fc2, fc3)" -> "Phono3py (LTC)";
"Phono3py (LTC)" -> "Lattice thermal conductivity";
}
}