.. _lattice:

.. automodule:: spintoolkit_py
    :no-index:

====================
Class
====================

.. autoclass:: spintoolkit_py.lattice
    :members:
    :undoc-members:
    :show-inheritance:
    :exclude-members: __init__, coor2cart

    .. method:: __init__(self)

        Default constructor.

    .. method:: __init__(self, *, basis_a: list[list[float]], pos_sub: list[list[float]], l: list[int])
        :no-index:

        Construct an untilted lattice (:math:`\boldsymbol{A}_j \parallel \boldsymbol{a}_j`) from a given basis.

        :param basis_a: Real-space basis vectors :math:`[\boldsymbol{a}_0, \boldsymbol{a}_1, \ldots]`.
        :param pos_sub: List of sublattice coordinates in units of the basis :math:`\boldsymbol{a}_j`.
        :param l: List of linear dimensions along each basis direction.

    .. method:: __init__(self, *, name: str, l: list[int])
        :no-index:

        Construct an untilted lattice (:math:`\boldsymbol{A}_j \parallel \boldsymbol{a}_j`) from a built-in name.

        :param name: Name of the lattice. Choose from [chain, square, triangular, kagome, honeycomb, cubic, fcc, triangular-stacked, pyrochlore, pyrochlore-16, pyrochlore-111].
        :param l: List of linear dimensions along each basis direction.

    .. method:: __init__(self, *, filename: str)
        :no-index:

        Construct a general lattice from a user-defined TOML file.

        :param filename: Name of the toml file.

        .. rubric:: Notes

        The TOML file must specify the lattice geometry and sublattice structure with the following fields:

        - ``dim`` : Spatial dimension (1, 2, or 3).
        - ``a0``, ``a1``, ``a2`` : Basis vectors :math:`\boldsymbol{a}_j` as floating-point arrays.
        - ``A0``, ``A1``, ``A2`` : Superlattice basis vectors :math:`\boldsymbol{A}_j` expressed as integer coefficients of the crystal basis.
        - ``num_sub`` : Number of sublattices.
        - ``pos_sub0``, ``pos_sub1``, ... : Sublattice coordinates in units of the basis :math:`\boldsymbol{a}_j`.
        - ``[[sub0]]``, ``[[sub1]]``, ... : Arrays of sublattice sites, where each entry contains a ``site`` field
          with integer coordinates specifying the position within the superlattice.

        The superlattice basis vectors :math:`\boldsymbol{A}_j` are not required to be parallel to the crystal
        basis vectors :math:`\boldsymbol{a}_j`, allowing for flexible magnetic unit cell definitions compatible
        with various ordering wave vectors.

        .. rubric:: Example

        Triangular lattice with 120° ordering (K-point):

        .. code-block:: toml

            dim = 2

            a0 = [ 1.0, 0.0 ]
            a1 = [ -0.5, 0.86602540378443865 ]

            A0 = [ 2, 1 ]
            A1 = [ 1, 2 ]

            num_sub = 1
            pos_sub0 = [ 0.0, 0.0 ]

            [[sub0]]
            site = [ 0, 0 ]
            [[sub0]]
            site = [ 1, 0 ]
            [[sub0]]
            site = [ 1, 1 ]

    .. method:: coor2cart(self, *, coor: list[int]) -> list[float]

        Calculate Cartesian coordinate :math:`[x,y,z]= \sum_i m_i \boldsymbol{a}_i` with given coordinate :math:`m_i`.

        :param coor: Coordinate :math:`[m_0, m_1, \ldots]`.
        :rtype: list[float]
        :return: Cartesian coordinate :math:`[x,y,z]`.

    .. method:: coor2cart(self, *, coor: list[int], sub: int) -> list[float]
        :no-index:

        Calculate Cartesian coordinates :math:`[x,y,z]= \sum_i m_i \boldsymbol{a}_i + \vec{d}` with
        given coordinate :math:`m_i` and sublattice index (:math:`\vec{d}` accounts for the displacement of the sublattice).

        :param coor: Coordinate :math:`[m_0, m_1, \ldots]`.
        :param sub: Index of sublattice.
        :rtype: list[float]
        :return: Cartesian coordinate :math:`[x,y,z]`.