Source code for httk.atomistic.wyckoff

"""Exact rational Wyckoff-position algebra.

A Wyckoff position is a family of symmetry-equivalent sites parameterised by a few free
coordinates: SG 15 letter ``e`` is ``0,y,1/4``, so one free parameter ``y`` places four
symmetry-equivalent atoms. This module goes both ways between free parameters and
coordinates, entirely over the rationals.

Two properties of the vendored tables make this much simpler than it looks, both asserted
in ``tests/test_symmetry_data.py``:

* Each Wyckoff position's ``orbit`` is already the **complete, deduplicated** list of
  affine maps, of length exactly ``multiplicity``, with centering translations folded in.
  Generating an orbit is therefore a plain loop with no coincidence testing and no
  tolerance.
* ``hasfreedom`` marks which of ``x``, ``y``, ``z`` are free, and the columns of every
  orbit matrix for the non-free variables are identically zero, with
  ``sum(hasfreedom) == rank``. So the free parameters are read straight off, and the
  ``first_orbit`` strings (``"1/8,y,-y+1/4"``) never need parsing — the same information
  is already present as an exact affine map.

Everything is expressed in the coordinates of whichever setting the record came from.
"""

import fractions
from collections.abc import Sequence
from typing import Any, Self

from httk.core import FracVector

from .affine_operation import AffineOperation

__all__ = ["WyckoffBranch", "WyckoffPosition", "wyckoff_positions"]


[docs] class WyckoffBranch: """One member of a Wyckoff position's orbit: an affine map of the free parameters. A position of multiplicity *m* has *m* branches. The representative branch is the first, but a coordinate may lie on any of them, which is why :meth:`WyckoffPosition.parameters_of` tries them all. """ _operation: AffineOperation _free: tuple[int, ...] _unimodular: FracVector _echelon: FracVector _pivot_inverse: FracVector def __init__(self, operation: AffineOperation, free: Sequence[int]) -> None: self._operation = operation self._free = tuple(free) self._unimodular, self._echelon = _row_hermite(operation.matrix, self._free) rank = len(self._free) if rank: pivot = [[self._echelon[row][column].to_fraction() for column in range(rank)] for row in range(rank)] self._pivot_inverse = FracVector.create(_invert_small(pivot)) else: self._pivot_inverse = FracVector.create(()) @property
[docs] def operation(self) -> AffineOperation: """The affine map from a full ``(x, y, z)`` parameter triple to this branch's coordinate.""" return self._operation
@property
[docs] def free(self) -> tuple[int, ...]: """Indices into ``(x, y, z)`` of the free parameters, ascending.""" return self._free
[docs] def coordinate(self, parameters: Any) -> FracVector: """The coordinate this branch places at the given free-parameter values. ``parameters`` has one entry per free parameter. Because the non-free columns of the matrix are zero, the values placed at the non-free positions are irrelevant. """ placed = [fractions.Fraction(0)] * 3 values = FracVector.create(parameters) if not self._free: # A fixed position has no parameters. FracVector has no zero-length shape, so # "no parameters" is the empty vector, whose dim reads as () or (0,). if values.dim not in ((), (0,)): raise ValueError(f"a fixed Wyckoff position takes no free parameters, got dim {values.dim}") return self._operation.apply(placed) if values.dim != (len(self._free),): raise ValueError(f"expected {len(self._free)} free parameter(s), got dim {values.dim}") for slot, index in enumerate(self._free): placed[index] = values[slot].to_fraction() return self._operation.apply(placed)
[docs] def parameters_of(self, coordinate: Any) -> FracVector | None: """The free-parameter values putting this branch on ``coordinate``, or ``None``. ``None`` means the coordinate does not lie on this branch — for *any* lattice translation, not merely the one given. That completeness is what the row-Hermite form buys: with ``U`` unimodular over the integers, ``A t = d (mod Z^3)`` holds iff ``U A t = U d (mod Z^3)``, and the zero rows of ``U A`` turn the lattice-membership question into "are these components integers?" with no search over translations. The returned parameters are reduced into ``[0, 1)``, which is canonical: the pivot block has determinant ``±1`` throughout the vendored tables, so the solution is unique modulo one. The result is verified by re-evaluating the branch, so a table that ever violated that assumption would yield a clean miss rather than a wrong answer. """ point = FracVector.create(coordinate) rank = len(self._free) mapped = (point - self._operation.vector) * self._unimodular.T() # Rows below the rank carry no free parameter, so they must already be lattice # translations for the coordinate to lie on this branch at all. Checking that first # is a cheap rejection for the common case of a coordinate that is simply elsewhere. for row in range(rank, 3): if mapped[row].to_fraction().denominator != 1: return None parameters = self._parameters_from_mapped(mapped) if self.coordinate(parameters).normalize() != point.normalize(): return None return parameters
[docs] def nearest_parameters(self, coordinate: Any) -> FracVector: """The free-parameter values putting this branch as close to ``coordinate`` as it goes. Unlike :meth:`parameters_of` this always returns a value: the free directions are solved exactly and any discrepancy is left in the *fixed* directions, where the branch's own coordinates win. It is the projection used when recognizing a measured structure, whose coordinates carry rounding and do not lie exactly on any position. The projection is taken along the branch's own lattice basis rather than being minimised in the cell metric, so for a strongly oblique cell it is a near-optimal rather than provably optimal choice. That is safe because the caller measures the resulting Cartesian displacement and rejects anything beyond its tolerance — the method can cost a match, never grant a wrong one. """ point = FracVector.create(coordinate) mapped = (point - self._operation.vector) * self._unimodular.T() return self._parameters_from_mapped(mapped)
def _parameters_from_mapped(self, mapped: FracVector) -> FracVector: """Back-substitute the free parameters out of ``U * (point - b)``.""" rank = len(self._free) if rank == 0: return FracVector.create(()) head = FracVector.create([mapped[row].to_fraction() for row in range(rank)]) return (head * self._pivot_inverse.T()).normalize()
[docs] class WyckoffPosition: """A Wyckoff position of one space-group setting: a letter and its orbit.""" _letter: str _multiplicity: int _site_symmetry: str _free: tuple[int, ...] _branches: tuple[WyckoffBranch, ...] def __init__(self, record: dict[str, Any]) -> None: self._letter = record["letter"] self._multiplicity = record["multiplicity"] self._site_symmetry = record["sitesym"] self._free = tuple(index for index, free in enumerate(record["hasfreedom"]) if free) self._branches = tuple(WyckoffBranch(AffineOperation.from_record(item), self._free) for item in record["orbit"]) if len(self._branches) != self._multiplicity: raise ValueError( f"Wyckoff position {self._letter!r} has {len(self._branches)} orbit entries " f"but multiplicity {self._multiplicity}" ) @classmethod
[docs] def from_record(cls, record: dict[str, Any]) -> Self: return cls(record)
@property
[docs] def letter(self) -> str: """The Wyckoff letter, e.g. ``"e"``. Bare, with no multiplicity prefix.""" return self._letter
@property
[docs] def multiplicity(self) -> int: """How many sites one set of free-parameter values generates in the unit cell.""" return self._multiplicity
@property
[docs] def site_symmetry(self) -> str: """The site-symmetry group in Hermann-Mauguin notation, e.g. ``"2"`` or ``"-1"``.""" return self._site_symmetry
@property
[docs] def free(self) -> tuple[int, ...]: """Indices into ``(x, y, z)`` of the free parameters.""" return self._free
@property
[docs] def free_count(self) -> int: """How many degrees of freedom the position has, from 0 for a fixed position to 3.""" return len(self._free)
@property
[docs] def branches(self) -> tuple[WyckoffBranch, ...]: """The orbit, one branch per equivalent site. Complete and already deduplicated.""" return self._branches
@property
[docs] def representative(self) -> WyckoffBranch: """The first orbit member, the one the tables print as ``first_orbit``.""" return self._branches[0]
[docs] def coordinates(self, parameters: Any) -> FracVector: """Every coordinate of the orbit, as an exact ``(multiplicity, 3)`` block. Not wrapped and not deduplicated: within one setting the tabulated orbit is already distinct, so wrapping is the caller's business (and matters only once a setting transform enters). """ return FracVector.create([branch.coordinate(parameters).to_fractions() for branch in self._branches])
[docs] def parameters_of(self, coordinate: Any) -> FracVector | None: """The free-parameter values placing *some* branch on ``coordinate``, or ``None``. Tries every branch, not only the representative. That matters: across the vendored tables, 11673 of the 20639 non-representative orbit members lie on a different branch than the representative, so a matcher that only tested ``first_orbit`` would reject a majority of legitimate orbit points. """ for branch in self._branches: parameters = branch.parameters_of(coordinate) if parameters is not None: return parameters return None
def __repr__(self) -> str: return f"WyckoffPosition({self._multiplicity}{self._letter}, sitesym={self._site_symmetry!r})"
[docs] def wyckoff_positions(record: dict[str, Any]) -> tuple[WyckoffPosition, ...]: """The Wyckoff positions of a setting record, most specific first. Ordered by ``(free_count, multiplicity, letter)`` so that the first match found when identifying a coordinate is the most specific position it lies on. Ties do not arise: positions are affine subspaces, so a coordinate on two distinct positions of the same dimension also lies on their lower-dimensional intersection, which is covered by an earlier entry. """ positions = [WyckoffPosition(entry) for entry in record["wyckoff"]] positions.sort(key=lambda position: (position.free_count, position.multiplicity, position.letter)) return tuple(positions)
def _invert_small(rows: list[list[fractions.Fraction]]) -> list[list[fractions.Fraction]]: """The exact inverse of a small square rational matrix, by Gauss-Jordan elimination. :meth:`~httk.core.FracVector.inv` covers only scalars and 3x3 matrices, but the pivot blocks here are 1x1 and 2x2 as well (a Wyckoff position with one or two degrees of freedom). The sizes are at most 3, so the plain algorithm is entirely adequate. """ size = len(rows) work = [list(row) + [fractions.Fraction(1 if i == j else 0) for j in range(size)] for i, row in enumerate(rows)] for column in range(size): pivot = next((r for r in range(column, size) if work[r][column] != 0), None) if pivot is None: raise ValueError("singular matrix: a Wyckoff pivot block must be invertible") work[column], work[pivot] = work[pivot], work[column] scale = work[column][column] work[column] = [value / scale for value in work[column]] for row in range(size): if row != column and work[row][column] != 0: factor = work[row][column] work[row] = [a - factor * b for a, b in zip(work[row], work[column])] return [row[size:] for row in work] def _row_hermite(matrix: FracVector, free: Sequence[int]) -> tuple[FracVector, FracVector]: """Row-reduce the free columns of an orbit matrix to echelon form over the integers. Returns ``(U, H)`` with ``U`` unimodular (integer, determinant ``±1``) and ``H = U * A`` in row echelon form, where ``A`` is ``matrix`` restricted to the free columns. Unimodularity is the point: it preserves the integer lattice, so a congruence modulo ``Z^3`` may be applied to ``H`` and ``U d`` instead of ``A`` and ``d`` without changing which coordinates satisfy it. Uses gcd-based elimination (integer row reduction), so no division is ever inexact. Orbit matrices are integer with entries in ``{-2, ..., 2}``, so the values stay tiny. """ rows = [[int(matrix[row][column].to_fraction()) for column in free] for row in range(3)] unimodular = [[1 if row == column else 0 for column in range(3)] for row in range(3)] pivot_row = 0 for column in range(len(free)): # Drive all entries below the pivot to zero by repeated gcd steps. for row in range(pivot_row + 1, 3): while rows[row][column] != 0: if abs(rows[pivot_row][column]) > abs(rows[row][column]) or rows[pivot_row][column] == 0: rows[pivot_row], rows[row] = rows[row], rows[pivot_row] unimodular[pivot_row], unimodular[row] = unimodular[row], unimodular[pivot_row] if rows[pivot_row][column] == 0: break factor = rows[row][column] // rows[pivot_row][column] rows[row] = [a - factor * b for a, b in zip(rows[row], rows[pivot_row])] unimodular[row] = [a - factor * b for a, b in zip(unimodular[row], unimodular[pivot_row])] if rows[pivot_row][column] != 0: pivot_row += 1 if pivot_row == 3: break return FracVector.create(unimodular), FracVector.create(rows)